Fluorenone is a three-ring polycyclic ketone

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Accurate spectroscopy of polycyclic aromatic compounds: from the rotational
spectrum of fluoren-9-one in the millimeter wave region to its infrared spectrum
Assimo Maris, Camilla Calabrese, Sonia Melandri, and Susana Blanco
Supplemental Material
Table I-SM.
Experimental rotational transition frequency (ν/MHz) lines of fluoren-9-one.
J”(K-1”)-J'(K-1')
ν
νexp.-νcalc. J”(K-1”, K+1”)-J'(K-1', K+1')a
ν
νexp.-νcalc.
24 (24) - 23 (23) 68458.54
-0.08
33 (18) - 32 (17)
66173.33
0.01
25 (24) - 24 (23) 69467.34
-0.06
34 (18) - 33 (17)
67165.88
-0.08
23 (23) - 22 (22) 65567.13
-0.02
35 (18) - 34 (17)
68156.00
0.05
22 (21) - 21 (20) 60793.18
0.19
36 (18) - 35 (17)
69143.00
0.00
23 (21) - 22 (20) 61801.85
0.12
37 (18) - 36 (17)
70126.78
-0.02
23 (20) - 22 (19) 59918.70
-0.04
29 (17) - 28 (16)
60285.52
0.00
24 (20) - 23 (19) 60927.10
0.06
30 (17) - 29 (16)
61283.11
0.02
25 (20) - 24 (19) 61935.03
0.02
31 (17) - 30 (16)
62278.44
0.01
26 (20) - 25 (19) 62942.62
0.08
32 (17) - 31 (16)
63271.25
-0.02
27 (20) - 26 (19) 63949.57
0.03
33 (17) - 32 (16)
64261.29
-0.02
28 (20) - 27 (19) 64956.00
0.10
34 (17) - 33 (16)
65248.17
-0.05
29 (20) - 28 (19) 65961.58
0.07
35 (17) - 34 (16)
66231.64
-0.02
30 (20) - 29 (19) 66966.27
0.02
36 (17) - 35 (16)
67211.27
0.03
31 (20) - 30 (19) 67969.99
0.01
37 (17) - 36 (16)
68186.59
0.05
32 (20) - 31 (19) 68972.52
-0.05
38 (17) - 37 (16)
69157.13
0.03
33 (20) - 32 (19) 69973.88
0.01
39 (17) - 38 (16)
70122.45
0.05
19 (19) - 18 (18) 54001.04
-0.02
31 (16) - 30 (15)
60366.61
0.00
20 (19) - 19 (18) 55009.78
-0.11
32 (16) - 31 (15)
61353.36
-0.01
25 (19) - 24 (18) 60050.56
-0.05
33 (16) - 32 (15)
62336.32
-0.07
26 (19) - 25 (18) 61057.34
-0.04
34 (16) - 33 (15)
63315.20
-0.04
27 (19) - 26 (18) 62063.40
-0.03
35 (16) - 34 (15)
64289.43
0.01
28 (19) - 27 (18) 63068.61
-0.02
36 (16) - 35 (15)
65258.36
-0.04
29 (19) - 28 (18) 64072.85
0.01
32 (15) - 31 (14)
59419.03
0.09
30 (19) - 29 (18) 65075.90
-0.01
33 (15) - 32 (14)
60391.80
0.00
31 (19) - 30 (18) 66077.63
-0.04
34 (15) - 33 (14)
61358.95
0.07
32 (19) - 31 (18) 67078.04
0.07
35 (15) - 34 (14)
62319.56
-0.11
19 (18) - 18 (17) 52118.29
-0.02
36 (15, 22) - 35 (14, 21)
63272.68
0.02
20 (18) - 19 (17) 53126.95
-0.07
36 (15, 21) - 35 (14, 22)
63273.56
0.02
25 (18) - 24 (17) 58165.07
-0.01
37 (15, 23) - 36 (14, 22)
64217.45
0.07
27 (18) - 26 (17) 60175.44
-0.02
37 (15, 22) - 36 (14, 23)
64219.39
0.09
28 (18) - 27 (17) 61179.04
0.01
27 (14) - 26 (13)
52577.06
0.02
29 (18) - 28 (17) 62181.27
-0.02
28 (14) - 27 (13)
53563.41
0.02
30 (18) - 29 (17) 63181.95
-0.11
29 (14) - 28 (13)
54545.41
0.07
31 (18) - 30 (17) 64181.15
0.02
30 (14) - 29 (13)
55522.37
0.09
32 (18) - 31 (17) 65178.30
0.00
a Asymmetry
degenerate K-1 transition doublets are indicated as J”(K-1”)-J'(K-1')
1
Table II-SM.
Vibrational properties of fluoren-9-one calculated at the B3LYP/cc-pVTZ level: C2v symmetry representation, harmonic and
anharmonic (fundamental and first overtones) wavenumbers (ν/cm-1), reduced masses (μ/u), force constants (k/mDyn Å-1), infrared
intensities (Int./km mol-1), a and vibro-rotational coupling constants (α/MHz). Harmonic approximation data are given also for the
MP2/cc-pVTZ level of calculation.
B3LYP
Q(01)
Q(02)
Q(03)
Q(04)
Q(05)
Q(06)
Q(07)
Q(08)
Q(09)
Q(10)
Q(11)
Q(12)
Q(13)
Q(14)
Q(15)
Q(16)
Q(17)
Q(18)
Q(19)
Q(20)
Q(21)
Q(22)
Q(23)
Q(24)
Q(25)
Q(26)
Q(27)
Q(28)
Q(29)
Q(30)
Q(31)
Q(32)
Q(33)
Q(34)
Q(35)
Q(36)
Q(37)
Q(38)
Q(39)
Q(40)
Q(41)
Q(42)
Q(43)
Q(44)
Q(45)
Q(46)
Q(47)
Q(48)
Q(49)
Q(50)
Q(51)
Q(52)
Q(53)
Q(54)
Q(55)
Q(56)
Q(57)
Q(58)
Q(59)
Q(60)
Γirr.
A1
B2
A1
B2
A1
B2
A1
B2
A1
B2
A1
B2
A1
A1
B2
B2
A1
A1
B2
B2
A1
A1
B2
A1
B2
A1
B2
A1
B2
A1
B2
B1
A2
B1
A2
B2
B1
A2
B1
A2
A1
B1
A2
A1
B1
B2
B2
A2
A1
B2
B1
A2
A1
B1
B2
A2
A1
B1
A2
B1
νharm.
μ
k
Int.
3195 1.10 6.60
0.9
3194 1.10 6.59 38.8
3186 1.09 6.54 26.1
3185 1.09 6.53
0.9
3178 1.09 6.48
2.9
3177 1.09 6.47
3.2
3168 1.09 6.42
0.1
3166 1.09 6.42
2.8
1784 12.86 24.12 257.8
1651 6.86 11.01 75.9
1637 6.45 10.18 29.7
1634 6.65 10.46
4.5
1628 5.52 8.63 18.7
1509 2.82 3.78
0.4
1508 2.48 3.32
1.3
1490 2.23 2.92 44.9
1478 2.49 3.21
0.8
1402 4.08 4.73
0.8
1329 3.07 3.20 38.7
1324 2.00 2.07 11.6
1315 1.72 1.76
3.5
1227 2.62 2.33
0.0
1207 2.68 2.29 43.0
1188 1.20 1.00
0.3
1181 1.20 0.99
3.4
1174 2.34 1.90 13.3
1117 1.83 1.35 25.6
1104 2.48 1.78
0.0
1057 1.99 1.31
0.2
1041 2.27 1.45
0.2
1025 5.28 3.27
0.9
1011 1.32 0.79
0.0
1009 1.32 0.79
982 1.44 0.81
2.5
978 1.40 0.79
933 7.24 3.71 53.4
907 1.44 0.70
0.1
906 1.49 0.72
840 3.04 1.26
4.3
807 2.47 0.95
790 6.28 2.31
0.1
760 1.41 0.48 109.4
763 1.54 0.53
739 5.79 1.86
0.0
694 4.25 1.21 14.7
668 6.90 1.81
4.8
634 7.08 1.68
1.6
574 3.29 0.64
567 8.68 1.65
0.6
513 5.69 0.88
2.7
460 4.26 0.53
4.3
440 3.13 0.36
413 6.59 0.66
0.1
412 3.21 0.32
0.8
285 9.41 0.45
5.0
271 4.75 0.21
206 4.63 0.12
0.2
150 7.10 0.09
0.4
132 3.81 0.04
98 4.67 0.03
2.6
νanh.
Int. νovertone Int.
3064
1.0 6119 0.02
3065 36.0 6094 0.02
3062 28.0 6120 0.00
3072
5.8 6130 0.00
3057
2.8 6079 0.00
3057
2.7 6104 0.00
3025
0.3 6063 0.41
3016
3.2 6041 0.59
1751 228.2 3484 5.03
1612 60.5 3222 0.00
1598
4.4 3194 0.07
1598
2.4 3194 0.23
1589 16.0 3180 0.18
1477
0.5 2951 0.00
1478
2.7 2952 0.01
1462 28.6 2921 0.03
1446
0.7 2892 0.00
1372
0.7 2742 0.04
1300 11.7 2599 0.16
1296 16.2 2590 0.01
1285
2.4 2577 0.02
1201
0.0 2399 0.01
1182 24.7 2363 0.19
1175
0.0 2351 0.01
1169
6.6 2339 0.04
1153
7.5 2305 0.00
1097 21.2 2193 0.13
1083
0.2 2174 0.00
1041
0.3 2081 0.00
1026
0.1 2050 0.00
1004
0.7 2016 0.00
1009
0.3 2023 0.07
1007
0.0 2018 0.09
966
0.4 1933 0.02
964
0.0 1930 0.11
918 49.6 1838 9.69
890
0.0 1780 0.04
897
0.0 1797 0.31
830
1.9 1659 0.74
811
0.0 1624 0.03
778
0.1 1556 0.00
753
0.2 1505 0.27
749 99.3 1497 0.01
727
0.0 1455 0.00
690 16.5 1380 0.22
661
4.1 1322 0.00
627
1.2 1254 0.00
573
0.0 1147 0.11
564
0.5 1119 0.02
505
2.4 1008 0.00
454
3.6
909 0.02
433
0.0
866 0.00
407
0.2
815 0.00
401
0.6
802 0.00
279
5.0
560 0.03
269
0.0
539 0.00
201
0.2
403 0.00
155
0.3
310 0.03
138
0.0
277 0.00
100
2.7
199 0.01
αa
0.23
0.23
0.18
0.20
0.18
0.20
0.14
0.15
2.32
0.88
0.93
0.84
0.69
0.54
0.04
0.72
0.10
0.69
0.99
0.47
-0.25
-0.26
1.98
-0.38
-0.05
1.10
0.20
-0.18
0.13
0.26
0.05
0.72
0.75
0.42
0.50
0.81
0.37
0.38
-0.14
0.27
0.21
0.29
0.32
-0.20
0.32
-0.30
-0.53
0.90
0.34
-0.24
-0.08
0.16
-0.04
0.17
-1.29
1.93
-1.96
-0.53
0.03
2.38
αb
0.06
0.06
0.09
0.08
0.08
0.07
0.07
0.07
0.08
0.54
0.52
0.36
0.50
0.32
0.27
0.04
0.33
0.55
0.34
0.14
0.37
0.60
0.14
0.08
0.02
0.11
0.11
0.13
-0.03
-0.01
0.12
0.13
0.11
0.12
0.12
0.09
0.05
0.06
0.13
-0.24
0.45
0.01
0.01
0.17
-0.24
0.18
0.12
-0.01
0.00
0.07
0.01
-0.14
0.11
-0.09
-0.27
-0.23
-0.25
0.14
0.23
-0.28
αc
0.05
0.05
0.06
0.05
0.06
0.05
0.05
0.05
0.22
0.01
0.52
0.27
0.50
0.24
0.18
-0.09
0.43
0.32
0.25
0.14
0.24
0.33
0.29
0.08
0.06
0.23
0.11
0.05
0.22
0.10
0.14
0.01
0.01
0.01
0.00
0.20
0.00
0.00
-0.01
-0.03
0.13
-0.03
-0.03
0.08
-0.04
0.09
0.06
-0.07
0.06
0.10
-0.09
-0.14
0.14
-0.13
0.02
-0.19
0.06
-0.21
-0.15
-0.28
MP2
Q(01)
Q(02)
Q(03)
Q(04)
Q(05)
Q(06)
Q(07)
Q(08)
Q(09)
Q(10)
Q(11)
Q(12)
Q(13)
Q(14)
Q(15)
Q(16)
Q(17)
Q(18)
Q(19)
Q(20)
Q(21)
Q(22)
Q(23)
Q(24)
Q(25)
Q(26)
Q(27)
Q(28)
Q(29)
Q(30)
Q(31)
Q(32)
Q(33)
Q(34)
Q(35)
Q(36)
Q(37)
Q(38)
Q(39)
Q(40)
Q(41)
Q(42)
Q(43)
Q(44)
Q(45)
Q(46)
Q(47)
Q(48)
Q(49)
Q(50)
Q(51)
Q(52)
Q(53)
Q(54)
Q(55)
Q(56)
Q(57)
Q(58)
Q(59)
Q(60)
Γirr.
A1
B2
A1
B2
A1
B2
A1
B2
A1
B2
A1
B2
A1
A1
B2
A1
B2
B2
A1
A1
B2
A1
B2
A1
B2
A1
B2
A1
B2
A1
B2
B1
A2
B1
A2
B2
B1
A2
B1
A1
A2
B1
A1
A2
B1
B2
B2
A1
A2
B2
B1
A2
A1
B1
B2
A2
A1
B1
A2
B1
ν harm.
μ
k
Int.
3236 1.10 6.78
1.4
3235 1.10 6.77 25.8
3225 1.09 6.71 13.7
3224 1.09 6.70
0.1
3217 1.09 6.64
2.0
3215 1.09 6.64
0.8
3206 1.09 6.58
0.0
3205 1.09 6.58
1.8
1759 12.93 23.59 159.6
1652 7.30 11.74 55.0
1647 7.18 11.46 22.2
1636 7.32 11.56
2.4
1636 6.35 10.02
4.1
1528 6.67 9.17
0.1
1501 2.70 3.58
8.0
1497 2.98 3.93
0.9
1477 2.33 2.99 44.7
1468 7.85 9.96
2.5
1452 2.39 2.97
1.9
1319 1.92 1.96
1.1
1317 1.68 1.72 55.5
1249 2.11 1.94
0.6
1228 2.52 2.24 48.0
1184 1.58 1.31
7.3
1178 1.11 0.91
5.1
1173 1.40 1.13
7.1
1120 1.63 1.21 15.8
1099 2.52 1.80
0.0
1049 1.81 1.17
0.1
1038 2.17 1.38
0.5
1017 6.25 3.80
2.8
969 1.21 0.67
0.1
967 1.23 0.68
948 1.37 0.73
2.1
944 1.34 0.71
924 7.20 3.62 43.6
887 1.28 0.59
0.0
879 1.27 0.58
799 2.42 0.91 30.8
780 6.17 2.21
0.0
771 1.36 0.48
741 1.88 0.61 92.5
730 5.70 1.79
0.1
707 5.42 1.60
663 5.89 1.53
8.8
653 6.86 1.72
5.4
617 7.02 1.58
1.6
561 8.64 1.60
0.2
557 3.82 0.70
509 5.75 0.88
1.5
446 4.47 0.52
3.7
421 3.33 0.35
411 6.59 0.66
0.1
399 3.38 0.32
0.9
276 9.28 0.42
4.8
265 4.83 0.20
200 4.62 0.11
0.2
144 7.17 0.09
0.1
128 3.82 0.04
94 4.67 0.02
2.6
a The conversion factor to cm molecule-1 is cf=6.023-1 10-18.
b Because of the C2v symmetry selection rules the A out-of-plane vibrational normal modes are not infrared active.
2
2
Table III-SM.
Vibrational properties of 9H-fluorene calculated at the B3LYP/cc-pVTZ level: C2v symmetry representation, harmonic and
anharmonic (fundamental and first overtones) wavenumbers (ν/cm-1), reduced masses (μ/u), force constants (k/mDyn Å-1), infrared
intensities (Int./km mol-1),a and vibro-rotational coupling constants (α/MHz).
Q(01)
Q(02)
Q(03)
Q(04)
Q(05)
Q(06)
Q(07)
Q(08)
Q(09)
Q(10)
Q(11)
Q(12)
Q(13)
Q(14)
Q(15)
Q(16)
Q(17)
Q(18)
Q(19)
Q(20)
Q(21)
Q(22)
Q(23)
Q(24)
Q(25)
Q(26)
Q(27)
Q(28)
Q(29)
Q(30)
Q(31)
Q(32)
Q(33)
Q(34)
Q(35)
Q(36)
Q(37)
Q(38)
Q(39)
Q(40)
Q(41)
Q(42)
Q(43)
Q(44)
Q(45)
Q(46)
Q(47)
Q(48)
Q(49)
Q(50)
Q(51)
Q(52)
Q(53)
Q(54)
Q(55)
Q(56)
Q(57)
Q(58)
Q(59)
Q(60)
Q(61)
Q(62)
Q(63)
Γirr
A1
B2
A1
B2
A1
B2
A1
B2
B1
A1
B2
A1
B2
A1
B2
A1
B2
A1
A1
A1
B2
B2
A1
A1
B2
A1
B2
A1
B2
A2
B2
A1
B2
A1
B2
B1
A2
B1
A2
B1
A2
B1
A1
B2
A2
B1
A1
A2
B1
A1
B2
A2
B2
B2
B1
A2
B1
A1
A2
B1
A1
A2
B1
νharm.
3190
3189
3178
3176
3167
3165
3160
3159
3045
3023
1650
1649
1624
1620
1515
1512
1490
1483
1452
1376
1347
1333
1325
1255
1223
1210
1195
1183
1179
1166
1133
1121
1056
1048
1029
996
994
980
957
938
887
877
856
815
804
759
758
747
717
646
638
581
555
500
486
441
425
420
277
245
217
138
99
μ
1.10
1.10
1.09
1.09
1.09
1.09
1.09
1.09
1.10
1.06
6.60
6.19
6.33
5.39
2.55
2.79
2.20
2.30
1.14
4.37
2.23
2.52
1.86
2.68
1.77
2.63
1.61
1.15
1.28
1.14
1.70
2.07
2.12
2.26
6.13
1.28
1.29
1.84
1.41
1.60
1.44
1.29
5.29
3.84
2.31
1.28
5.35
1.52
2.99
6.14
6.93
3.46
5.63
4.11
2.93
2.87
2.86
6.46
4.45
2.14
4.37
3.69
4.27
k
6.57
6.57
6.50
6.49
6.43
6.42
6.39
6.39
6.02
5.70
10.58
9.91
9.83
8.34
3.45
3.76
2.88
2.98
1.42
4.88
2.39
2.64
1.92
2.49
1.56
2.27
1.36
0.95
1.05
0.92
1.29
1.53
1.39
1.47
3.82
0.75
0.75
1.04
0.76
0.83
0.67
0.59
2.29
1.50
0.88
0.43
1.81
0.50
0.91
1.51
1.66
0.69
1.02
0.60
0.41
0.33
0.31
0.67
0.20
0.08
0.12
0.04
0.02
Int.
4.8
48.4
40.8
5.2
4.1
1.9
8.3
2.8
8.2
15.2
3.5
0.0
0.2
1.4
7.8
0.1
19.9
10.0
10.9
0.3
5.6
4.0
0.2
3.4
3.4
2.2
3.6
0.0
0.3
0.2
2.5
4.1
0.6
3.8
0.0
3.5
0.0
0.7
0.1
0.3
111.5
0.0
5.8
0.3
7.5
0.1
0.3
0.8
5.6
0.4
6.5
0.2
0.5
αa
0.43
0.44
0.36
0.39
0.32
0.34
0.39
0.38
0.05
0.24
1.49
1.42
1.55
1.46
0.18
1.10
0.99
0.06
0.38
1.27
1.16
1.27
-0.16
0.73
1.23
0.41
0.02
-0.50
-0.09
1.24
0.17
-0.61
0.57
0.79
0.04
1.46
1.54
0.90
1.13
0.47
0.52
-0.30
1.16
0.09
1.14
0.66
-0.32
0.79
-0.35
1.10
-1.47
1.32
0.55
-1.98
0.17
0.64
0.41
-0.27
2.16
-0.51
-3.46
0.29
5.10
αb
0.06
0.06
0.09
0.08
0.10
0.10
0.07
0.07
0.01
0.02
0.52
0.60
0.33
0.38
0.27
0.34
0.09
0.29
-0.01
0.64
0.24
0.25
0.43
0.49
0.07
0.24
0.15
0.03
0.00
0.06
0.12
0.17
-0.07
0.00
0.13
0.11
0.09
0.11
0.09
0.06
0.05
0.05
0.12
0.14
0.01
0.01
0.25
-0.01
-0.01
0.01
0.06
-0.01
0.01
0.05
0.01
-0.12
-0.08
0.11
-0.20
0.03
-0.26
0.28
-0.39
αc
0.05
0.05
0.07
0.06
0.07
0.07
0.06
0.06
0.01
0.01
0.11
-0.06
0.83
0.60
0.22
0.31
0.12
0.23
-0.04
0.39
0.28
0.26
0.32
0.39
0.17
0.25
0.16
0.08
0.12
-0.03
0.10
0.14
0.20
0.13
0.18
0.01
0.01
0.03
-0.01
0.00
0.00
0.01
0.04
0.24
-0.03
-0.03
0.17
-0.05
-0.01
0.08
0.07
-0.08
0.10
0.07
-0.08
-0.15
-0.14
0.16
-0.21
-0.11
0.03
-0.14
-0.40
νanh.
3051
3052
3046
3047
3032
3030
3010
3009
2891
2903
1610
1607
1584
1581
1482
1478
1459
1452
1411
1349
1312
1302
1293
1223
1189
1187
1173
1162
1159
1135
1111
1099
1034
1027
1011
1004
1004
974
962
927
878
860
842
802
799
748
748
741
721
638
632
579
549
491
482
438
421
416
272
244
208
130
98
Int.
0.1
66.0
80.5
10.1
86.8
19.9
83.3
7.9
10.5
17.1
1.0
0.1
0.5
0.8
2.9
0.2
17.2
8.5
7.6
0.1
1.9
4.2
0.1
3.0
1.6
2.1
4.1
0.1
0.0
0.0
0.6
1.9
1.2
0.3
4.5
0.4
0.0
4.4
0.0
0.0
0.0
0.6
0.1
0.2
0.0
100.1
0.0
0.0
17.4
0.2
7.1
0.0
0.1
0.3
0.8
0.0
5.9
0.3
0.0
5.9
0.2
0.0
0.6
a The conversion factor to cm molecule-1 is cf=6.023-1 10-18.
b Because of the C2v symmetry selection rules the A out-of-plane vibrational normal modes are not infrared active.
2
3
νovertone
6069
6091
6079
6096
6051
6039
6010
6041
5714
5698
3221
3213
3173
3162
2960
2954
2916
2901
2796
2695
2620
2601
2585
2450
2380
2372
2346
2327
2318
2263
2222
2198
2067
2053
2022
2018
2012
1949
1929
1854
1757
1719
1685
1603
1599
1496
1496
1481
1443
1276
1265
1158
1098
981
965
877
842
831
544
489
416
259
194
Int.
0.02
0.02
0.06
0.06
0.20
0.17
0.11
0.04
1.17
0.32
0.00
0.00
0.25
0.23
0.00
0.02
0.00
0.00
0.20
0.01
0.02
0.00
0.01
0.01
0.01
0.00
0.00
0.05
0.05
0.18
0.00
0.00
0.00
0.00
0.00
0.40
0.33
0.07
0.20
0.43
0.15
0.07
0.00
0.01
0.00
0.03
0.05
0.11
0.19
0.00
0.01
0.00
0.00
0.00
0.01
0.02
0.00
0.00
0.01
0.02
0.00
0.00
0.00
Extended references list
[1]
A toxicological review of polycyclic aromatic hydrocarbons. R.W. Pickering, Cutan. Ocul. Toxicol., 18 (1999) 101-135.
DOI: 10.3109/15569529909037562
[2]
Sources, Fate, and Toxic Hazards of Oxygenated Polycyclic Aromatic Hydrocarbons (PAHs) at PAH-contaminated Sites. S. Lundstedt, P.A.
White, C.L. Lemieux, K.D. Lynes, I.B. Lambert, L. Öberg, P. Haglund, and M. Tysklind. AMBIO, 36 (2007) 475-485.
DOI: 10.1579/0044-7447(2007)36[475:SFATHO]2.0.CO;2
[3]
Large polycyclic aromatic hydrocarbons: Synthesis and discotic organization. X. Feng, W. Pisula, and K. Müllen, Pure Appl. Chem., 81
(2009) 2203-2224.
DOI: 10.1351/PAC-CON-09-07-07.
[4]
Revisiting Fluorenone Photophysics via Dipolar Fluorenone Derivatives. L.A. Estrada, J.E. Yarnell, and D.C. Neckers, J. Phys. Chem. A,
115 (2011) 6366-6375.
DOI: 10.1021/jp200507j
[5]
Ultrafast Hydrogen Bond Strengthening of the Photoexcited Fluorenone in Alcohols for Facilitating the Fluorescence Quenching. G.-J.
Zhao, and K.-L. Han, J. Phys. Chem. A, 111 (2007) 9218-9223.
DOI: 10.1021/jp0719659
[6]
A fluorenone based low band gap solution processable copolymer for air stable and high mobility organic field effect transistors. P. Sonar,
T.-J. Hab, and A. Dodabalapur, Chem. Commun., 49 (2013) 1588.
DOI: 10.1039/c2cc37131f
[7]
PAHs in Astronomy - A Review. F. Salama, Proc. IAU Symp. S251, 4 (2008) 357-366.
DOI: 10.1017/S1743921308021960
[8]
Identification of the 'unidentified' IR emission features of interstellar dust? A. Leger, and J.L. Puget, A&A, 137 (1984) L5-L8.
http://adsabs.harvard.edu/abs/1984A%26A...137L...5L
[9]
Polycyclic aromatic hydrocarbons and the unidentified infrared emission bands. L.J. Allamandola, A.G.G.M. Tielens, and J.R. Barker, ApJ,
290 (1985) L25-L28.
DOI: 10.1086/184435
[10]
Interstellar Polycyclic Aromatic Hydrocarbon Molecules. A.G.G.M. Tielens, Annu. Rev. Astro. Astrophys. 46 (2008) 289-337.
DOI: 10.1146/annurev.astro.46.060407.145211
[11]
Mixed aromatic-aliphatic organic nanoparticles as carriers of unidentified infrared emission features. S. Kwok, and Y. Zhang, Nature 479
(2011) 80-83.
DOI: 10.1038/nature10542.
[12]
The carriers of the interstellar Unidentified Infrared Emission features: constraints from interstellar C-H stretching features at 3.2-3.5 μm.
X.J. Yang, R. Glaser, A. Li, and J.X. Zhong, ApJ 776 (2013) 110 1-6.
DOI: 10.1088/0004-637X/776/2/110
[13]
The carriers of the interstellar Unidentified Infrared Emission features: aromatic or aliphatic? A. Li, and B.T. Draine, ApJL, 760 (2012) L35
1-5.
DOI: 10.1088/2041-8205/760/2/L35
[14]
The molecular universe. A.G.G.M. Tielens, Rev. Mod. Phys. 85 (2013) 1021-1081.
DOI: 10.1103/RevModPhys.85.1021
[15]
Far-Infrared Spectroscopy of Cationic Polycyclic Aromatic Hydrocarbons: Zero Kinetic Energy Photoelectron Spectroscopy of Pentacene
Vaporized from Laser Desorption. J. Zhang, F. Han, L. Pei, W. Kong, and A. Li, ApJ, 715 (2010) 485-492.
DOI: 10.1088/0004-637X/715/1/485 Vibro-Rot alpha Matrix (in MHz)
[16]
A general model for the identification of specific PAHs in the far-IR. G. Mulas, G. Malloci, C. Joblin, and D. Toublanc. A&A, 460 (2006) 93104.
DOI: 10.1051/0004-6361:20054276
[17]
Diagnostics for specific PAHs in the far-IR: searching neutral naphthalene and anthracene in the Red Rectangle. G. Mulas, G. Malloci, C.
Joblin, and D. Toublanc, A&A 456 (2006) 161-169.
DOI: 10.1051/0004-6361:20065435
[18]
Interstellar Chemistry: A Strategy for Detecting Polycyclic Aromatic Hydrocarbons in Space. F.J. Lovas, R.J. McMahon, J.-U. Grabow, M.
Schnell, J. Mack, L.T. Scott, and R.L. Kuczkowski, J. Am. Chem. Soc., 127 (2005) 4345-4349.
DOI: 10.1021/ja0426239
[19]
Rotational Spectra of Small PAHs: Acenaphthene, Acenaphthylene, Azulene, and Fluorene. S. Thorwirth, P. Theulé, C.A. Gottlieb, M.C.
McCarthy, and P. Thaddeus, ApJ, 662 (2007) 1309-1314.
DOI: 10.1086/518026
[20]
Microwave spectrum and 14N quadrupole coupling constants of carbazole. R. D. Suenram, F.J. Lovas, G.T. Fraser, and P.S. Marfey, J. Mol.
Struct., 190 (1988) 135-141.
DOI: 10.1016/0022-2860(88)80278-3
[21]
Millimetre wave spectroscopy of PANHs: phenanthridine. D. McNaughton, P.D. Godfrey, R.D. Brown, and S. Thorwirth, Phys. Chem. Chem.
Phys., 9 (2007) 591-595.
DOI: 10.1039/b615485a
4
[22]
FT-MW and Millimeter Wave Spectroscopy of PANHs: Phenanthridine, Acridine, and 1,10-Phenanthroline. D. McNaughton, P.D. Godfrey,
R.D. Brown, S. Thorwirth, and J.-U. Grabow, ApJ, 678 (2008) 309-315.
DOI: 10.1086/529430
[23]
Structural Characterization of 9-Cyanoanthracene-(Ar)n (n = 0-3) by Rotational Coherence Spectroscopy. K. Egashira, Y. Ohshima, and O.
Kajimoto, J. Phys. Chem. A, 105 (2001) 1131-1139.
DOI; 10.1021/jp0035378
[24]
FTMW and millimeter wave spectroscopy of benzanthrone. D. McNaughton, P.D. Godfrey, and J.-U. Grabow, J. Mol. Spectrosc., 274 (2012)
1-4.
DOI: 10.1016/j.jms.2012.03.003
[25]
The Nature and Distribution of the Organic Material in Carbonaceous Chondrites and Interplanetary Dust Particles. S. Pizzarello, G.W.
Cooper, and G.J. Flynn, in: Meteorites and the Early Solar System II, ed. D.S. Lauretta and H.Y. McSween, The University of Arizona Press.
http://www.lpi.usra.edu/books/MESSII/9008.pdf
[26]
Ultraviolet irradiation of naphthalene in H2O ice: Implications for meteorites and biogenesis. M.P. Bernstein, J.P. Dworkin, S.A. Sandford,
and L.J. Allamandola, Meteorit. Planet. Sci. 36 (2001) 351-358.
DOI: 10.1111/j.1945-5100.2001.tb01878.x
[27]
UV photolysis of quinoline in interstellar ice analogs. J.E. Elsila, M.R. Hammond, M.P. Bernstein, S.A. Sandford, and R.N. Zare, Meteorit.
Planet. Sci. 41 (2006) 785-796.
DOI: 10.1111/j.1945-5100.2006.tb00992.x
[28]
Über das Elektronenspektrum von Fluorenon. Beobachtung einer durch ein elektrisches Feld induzierten Absorptionsbande (On the
electronic spectrum of fluorenone. Observation induced by an electric field absorption band). W. Liptay, H. Weisenberger, F. Tiemann, W.
Eberlein, and G. Konopka, Z. Naturforsch, 23A (1968) 377-393.
[29]
Free jet absorption millimeter wave spectrum of benzophenone. A. Maris, S. Melandri, W. Caminati, and P.G. Favero, Chem. Phys. Letters,
256 (1996) 509-512.
DOI: 10.1016/0009-2614(96)00467-8.
[30]
Vibrational analysis of fluorene. K. Witt, Spectrochim. Acta, 24A (1968) 1115-1123.
DOI: 10.1016/0584-8539(68)80131-X
[31]
Vibrational Assignment of Fluorene from the Infrared and Raman Spectra. A. Bree and R. Zwarich, J. Chem. Phys., 51 (1969) 912-920.
DOI: 10.1063/1.1672155
[32]
Theoretical Prediction of the Vibrational Spectrum of Fluorene and Planarized Poly(p-phenylene). L. Cuff and M. Kertesz, J. Phys. Chem.
98 (1994) 12223-12231.
DOI: 10.1021/j100098a017
[33]
Density Functional Theory Study of Vibrational Spectra of Fluorene. S.Y. Lee, B.H. Boo, J. Phys. Chem. 100 (1996) 8782-8785.
DOI: 10.1021/jp960020g
[34]
Vibrational spectra of fluorene, 1-methylfluorene and 1,8-dimethylfluorene. S. Chakraborty, P. Das, S. Manogaran, P.K. Das, Vib. Spectrosc.,
68 (2013) 162-169.
DOI: 10.1016/j.vibspec.2013.07.001
[35]
The vibrational spectra of 9-fluorenone. R. Zwarich, A. Bree, and V. Vilkos, J. Mol. Spectrosc., 51 (1974) 38-49.
DOI: 10.1016/0022-2852(74)90168-4
[36]
Molecular Structure and Vibrational Spectra of 9-Fluorenone Density Functional Theory Study. S.Y. Lee and B.H. Boo, Bull. Korean Chem.
Soc., 17 (1996) 760-764.
DOI: 10.1002/chin.199713014
[37]
Electronic and Vibrational Properties of Fluorenone in the Channels of Zeolite L. A. Devaux, C. Minkowski, and G. Calzaferri, Chem. Eur.
J., 10 (2004) 2391-2408.
DOI: 10.1002/chem.200305673
[38]
S. Califano in: Vibrational States, Wiley, London (1976).
[39]
Vibrational self-consistent field calculations for spectroscopy of biological molecules: new algorithmic developments and applications. T.K.
Roy and R.B. Gerber, Phys. Chem. Chem. Phys., 15 (2013) 9468-9492.
DOI: 10.1039/c3cp50739
[40]
General Atomic and Molecular Electronic Structure System. M.W. Schmidt, K.K. Baldridge, J.A. Boatz, S.T. Elbert, M.S. Gordon, J.H.
Jensen, S. Koseki, N. Matsunaga, K.A. Nguyen, S.J. Su, T.L. Windus, M. Dupuis, J.A. Montgomery, J. Comput. Chem., 14 (1993) 13471363.
DOI: 10.1002/jcc.540141112
[41]
Advances in electronic structure theory: GAMESS a decade later. M.S. Gordon, M.W. Schmidt pp. 1167-1189, in "Theory and Applications
of Computational Chemistry: the first forty years" C.E. Dykstra, G. Frenking, K.S. Kim, G.E. Scuseria (editors), Elsevier, Amsterdam
(2005).
[42]
Molpro: a general-purpose quantum chemistry program package. H.-J. Werner, P. J. Knowles, G. Knizia, F. R. Manby and M. Schütz,
WIREs Comput. Mol. Sci. 2 (2012) 242-253.
DOI: 10.1002/wcms.82
5
[43]
Anharmonic vibrational properties by a fully automated second-order perturbative approach. V. Barone, J. Chem. Phys., 122 (20055)
014108/1-15.
DOI: 10.1063/1.1824881
[44]
A second-order perturbation theory route to vibrational averages and transition properties of molecules: General formulation and
application to infrared and vibrational circular dichroism spectroscopies. J. Bloino and V. Barone, J. Chem. Phys., 136 (2012) 124108/1-15.
DOI: 10.1063/1.3695210.
[45]
Gaussian 09, Revision D.01, M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman, G. Scalmani,
V.Barone, B. Mennucci, G. A. Petersson, H. Nakatsuji, M. Caricato, X. Li, H. P. Hratchian, A. F. Izmaylov, J. Bloino, G. Zheng, J.
L.Sonnenberg, M. Hada, M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida, T. Nakajima, Y. Honda, O. Kitao, H. Nakai, T. Vreven,
J.A. Montgomery, Jr., J. E. Peralta, F. Ogliaro, M. Bearpark, J. J. Heyd, E. Brothers, K. N. Kudin, V. N. Staroverov, T. Keith, R. Kobayashi, J.
Normand, K. Raghavachari, A. Rendell, J. C. Burant, S. S. Iyengar, J. Tomasi, M. Cossi, N. Rega, J. M. Millam, M. Klene, J. E. Knox, J. B.
Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gomperts, R. E. Stratmann, O. Yazyev, A. J. Austin, R. Cammi, C. Pomelli, J. W. Ochterski, R.
L. Martin, K. Morokuma, V. G. Zakrzewski, G. A. Voth, P. Salvador, J. J. Dannenberg, S. Dapprich, A. D. Daniels, O. Farkas, J. B. Foresman,
J. V. Ortiz, J. Cioslowski, and D. J. Fox, Gaussian, Inc., Wallingford CT, 2013.
[46]
A microwave free jet absorption spectrometer and its first applications. S. Melandri, W. Caminati, L.B. Favero, A. Millemaggi, and P.G.
Favero, J. Mol. Struct. 352/353 (1995) 253-258.
DOI: 10.1016/0022-2860(94)08516-K
[47]
Observation of the rotational spectra of van der Waals complexes by free jet absorption millimeter wave spectroscopy: pyridine-argon. S.
Melandri, G. Maccaferri, A. Maris, A. Millemaggi, W. Caminati, and P.G. Favero, Chem. Phys. Lett., 261 (1996) 267-271.
DOI: 10.1016/0009-2614(96)00977-3
[48]
Keto-Enol Tautomerism and Conformational Landscape of 1,3-Cyclohexanedione from Its Free Jet Millimeter-Wave Absorption Spectrum. C.
Calabrese, A. Maris, L. Evangelisti, L.B. Favero, S. Melandri, and W. Caminati, J. Phys. Chem. A, 117 (2013) 13712-13718.
DOI: 10.1021/jp4078097
[49]
Experimental and Computational Study of the Thermodynamic Properties of 9-Fluorenone and 9-Fluorenol. M.J.S. Monte, R. Notario,
M.M.G. Calvinho, A.R.R.P. Almeida, L.M.P.F. Amaral, and A.I.M.C. Lobo Ferreira, M.D.M.C. Ribeiro da Silva, J. Chem. Eng. Data, 57
(2012) 2486-2496.
DOI: 10.1021/je300584m
[50]
Self-Consistent Equations Including Exchange and Correlation Effects. W. Kohn, and L.J. Sham, Phys. Rev., 140 (1965) A1133-A1138.
DOI: 10.1103/PhysRev.140.A1133
[51]
Note on an Approximation Treatment for Many-Electron Systems. C. Møller, and M.S. Plesset, Phys. Rev., 46 (1934) 618-622.
DOI: 10.1103/PhysRev.46.618
[52]
MP2 energy evaluation by direct methods. M. Head-Gordon, J.A. Pople, and M.J. Frisch, Chem. Phys. Lett., 153 (1988) 503-506.
DOI: 10.1016/0009-2614(88)85250-3.
[53]
Density-functional thermochemistry. III. The role of exact exchange. A.D. Becke, J. Chem. Phys., 98 (1993) 5648-5652.
DOI: 10.1063/1.464913
[54]
Development of the Colle-Salvetti correlation-energy formula into a functional of the electron density. C. Lee, W. Yang, and R.G. Parr, Phys.
Rev. B, 37 (1988) 785-789.
DOI: 10.1103/PhysRevB.37.785
[55]
Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen. T.H. Dunning Jr., J. Chem.
Phys., 90 (1989) 1007-1023.
DOI: 10.1063/1.456153
[56]
Accurate correlation consistent basis sets for molecular core-valence correlation effects: The second row atoms Al-Ar, and the first row
atoms B-Ne revisited. K.A. Peterson, and T.H. Dunning Jr., J. Chem. Phys., 117 (2002), 10548-10560.
DOI: 10.1063/1.1520138
[57]
NIST Recommended Rest Frequencies for Observed Interstellar Molecular Microwave Transitions - 2002 Revision. F. J. Lovas, J. Phys.
Chem. Ref. Data, 33 (2004) 177-355.
DOI: 10.1063/1.1633275
[58]
Spectral Evolution of the GRB 030329 Afterglow: Detection of the Supernova Nebular Phase Emissions. N. Kaifu, M. Ohishi, K. Kawaguchi,
S. Saito, S. Yamamoto, T. Miyaji, K. Miyazawa, S.-I. Ishikawa, C. Noumaru, S. Harasawa, M. Ocuda, and H. Suzuki, Publ. Astron. Soc. Jpn.,
56 (2004) 69-173.
DOI: 10.1093/pasj/56.1.61
[59]
The Millimeter and Submillimeter Spectrum of CRL 618. J.R. Goicoechea, J. Cernicharo, J.R. Pardo, M. Guelin, and T.G. Phillips, in: The
Promise of the Herschel Space Observatory, European Space Association, Vol. SP-460 (2001).
[60] IAU Commission 34 / Division VI - Astrochemistry Working Group, and web resources linked.
http://www.strw.leidenuniv.nl/iau34/
[61]
The GBT PRIMOS Project: Searching for our Molecular Origins, J.M. Hollis, A.J. Remijan, P.R. Jewell and F.J. Lovas.
http://www.cv.nrao.edu/~aremijan/PRIMOS/
[62]
Complete 2mm Spectral Line Survey (130-170 GHz) of Sgr B2N, Sgr B2OH, IRC +10 216, Orion (KL), Orion-S, W51M, and W3(IRS5),
arXiv:0802.2273 [astro-ph], A.J. Remijan, D.P. Leigh, A.J. Markwick-Kemper and B.E. Turner.
http://www.cv.nrao.edu/Turner2mmLineSurvey/
6
[63]
The fitting and prediction of vibration-rotation spectra with spin interactions. H.M. Pickett, J. Mol. Spectrosc., 148 (1991) 371-377.
DOI: 10.1016/0022-2852(91)90393-O
[64]
The crystal and molecular structure of 9-fluorenone. H.R. Luss, and D.L. Smith, Acta Cryst., B28 (1972) 884-889.
DOI: 10.1107/S056774087200336X
[65]
Über die Eigenwerte des asymmetrischen Kreisels. B.S.Ray, Z. Phys., 78 (1932) 74-91.
DOI: 10.1007/BF01342264
[66]
J.K.G. Watson, in: Vibration Spectra and Structure, vol. 6, ed. J. Durig, Elsevier, Amsterdam (1977), p. 1.
[67]
Microwave Molecular Spectra, ed. W. Gordy & R. L. Cook, Wiley, New York (1984).
[68]
On negative inertial defect. T. Oka, J. Mol. Struct., 352/353 (1995) 225-233.
DOI: 10.1016/0022-2860(95)08844-L
[69]
I.M. Mills, in: Molecular Spectroscopy: Modern Research, ed. K.N. Rao and C.W. Mathews, Academic, New York, (1972).
[70]
Laboratory rotational spectrum of acrylic acid and its isotopologues in the 6-18.5 GHz and 52-74.4 GHz frequency ranges. C. Calabrese, A.
Vigorito, G. Feng, L.B. Favero, A. Maris, S. Melandri, W.D. Geppert, and W. Caminati, J. Mol. Spectrosc., 295 (2014) 37-43.
DOI: 10.1016/j.jms.2013.11.003
[71]
NIST Chemistry WebBook
http://webbook.nist.gov/chemistry
7
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