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especially pp 3539-3543
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Randić, M. Chem. Rev. 2003, 103, 3449-3605; especially pp 3539-3543.
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80855159375
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In press. DOI: 10.1002/qua.23081
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Randić, M.; Nović, M.; Vračko, M; Vukičević, D.; Plavšić, D. Int. J. Quantum Chem. In press. DOI: 10.1002/qua.23081.
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Randić, M.1
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Plavšić, D.5
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23
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80755181764
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It should be noted that, despite its authorship, ref 14g is actually a historical paper reporting previously unpublished work (dating from 1953) by the late Professor C. A. Coulson, F.R.S. in which the London theory (14i) of diamagnetic susceptibility in conjugated systems is couched in terms of Coulson's own contour-integral formalism. (14j)
-
It should be noted that, despite its authorship, ref 14g is actually a historical paper reporting previously unpublished work (dating from 1953) by the late Professor C. A. Coulson, F.R.S., in which the London theory (14i) of diamagnetic susceptibility in conjugated systems is couched in terms of Coulson's own contour-integral formalism. (14j)
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26
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0011627997
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D. Phil. Thesis, University of Oxford (Linacre College): England, United Kingdom
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Gomes, J. A. N. F. Some Magnetic Effects in Molecules. D. Phil. Thesis, University of Oxford (Linacre College): England, United Kingdom, 1976; pp 69 - 73.
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Randić, M.; Plavšić, D; Vukičević, D. J. Indian Chem. Soc. 2011, 88, 13-23
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Plavšić, D.2
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34
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77955762423
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Balaban, A. T.; Dickens, T. K.; Gutman, I.; Mallion, R. B. Croatica Chem. Acta 2010, 83, 209-215
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Balaban, A.T.1
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Gutman, I.3
Mallion, R.B.4
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38
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80755181766
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Cambridge University Press: Cambridge, England, United Kingdom, S. M. P. Further Mathematics Series
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Smart, D. Linear Algebra & Geometry; Cambridge University Press: Cambridge, England, United Kingdom, 1988; S. M. P. Further Mathematics Series, pp 307-308.
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Linear Algebra & Geometry
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Smart, D.1
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40
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84945026192
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Baer, F.; Kuhn, H.; Regel, W. Z. Naturforsch. A 1967, 22, 103-112
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Z. Naturforsch. A
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Baer, F.1
Kuhn, H.2
Regel, W.3
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41
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80755149732
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-
In view of the theoretical formulation of the method proposed by Gomes, (17-19) this rule-printed in the text in italics -is here given a wording that is more general than that adopted for the corresponding rule (iii) in ref 16. (The original wording in ref 16 was "(iii) If at least one bond of a particular ring forms a part of a given "conjugation circuit", this ring shall be said to "participate" in that "conjugation circuit."'). Professor P. W. Fowler (36b, 36c) has recently proposed an equivalent version of rule (iii) that is couched entirely in terms of bond currents, rather than ring currents
-
In view of the theoretical formulation of the method proposed by Gomes, (17-19) this rule-printed in the text in italics -is here given a wording that is more general than that adopted for the corresponding rule (iii) in ref 16. (The original wording in ref 16 was "(iii) If at least one bond of a particular ring forms a part of a given "conjugation circuit", this ring shall be said to "participate" in that "conjugation circuit."'). Professor P. W. Fowler (36b, 36c) has recently proposed an equivalent version of rule (iii) that is couched entirely in terms of bond currents, rather than ring currents
-
-
-
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42
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80755181771
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Personal Communication, June 19th
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Fowler, P. W. Personal Communication, June 19th, 2011.
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(2011)
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Fowler, P.W.1
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46
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80755181769
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Even more elaborate "normalizations" have been discussed and argued for by Randić (40b) in the context, specifically, of structures related to perylene
-
Even more elaborate "normalizations" have been discussed and argued for by Randić (40b) in the context, specifically, of structures related to perylene
-
-
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47
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80755146950
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Personal communication to R.B.M. May 3
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Randić, M. Personal communication to R.B.M., May 3, 2011.
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(2011)
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48
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80755151369
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Personal communication, July 3
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Fowler, P. W. Personal communication, July 3, 2011.
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(2011)
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Fowler, P.W.1
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50
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0001539599
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Longuet-Higgins, H. C.; Salem, L. Proc. R. Soc. London, Ser. A 1960, 257, 445-456
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Longuet-Higgins, H.C.1
Salem, L.2
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53
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80755181772
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idem ibid
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idem ibid. 3635-3655.
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58
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80755149729
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Kirchhoff's Law of current conservation (26-29) is, by contrast, not violated in, for example, the " coupled Hartree-Fock" procedure described in
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Kirchhoff's Law of current conservation (26-29) is, by contrast, not violated in, for example, the " coupled Hartree-Fock" procedure described in
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59
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0000465059
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Coulson, C. A.; Gomes, J. A. N. F.; Mallion, R. B. Mol. Phys. 1975, 30, 713-732
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Mol. Phys.
, vol.30
, pp. 713-732
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Coulson, C.A.1
Gomes, J.A.N.F.2
Mallion, R.B.3
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62
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80755151366
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Personal communication to R. B. M. June 8
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Fowler, P. W. Personal communication to R. B. M., June 8, 2011.
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(2011)
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Fowler, P.W.1
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63
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80755146964
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Personal Communication to R. B. M. at the Fifth Conference on Computers in Scientific Discovery, Sheffield, England, United Kingdom, July
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Fowler, P. W.; Bean, D. E. Personal Communication to R. B. M. at the Fifth Conference on Computers in Scientific Discovery, Sheffield, England, United Kingdom, July 2010.
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(2010)
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Fowler, P.W.1
Bean, D.E.2
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66
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0001673919
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Haddon, R. C.; Haddon, V. R.; Jackman, L. M. Top. Curr. Chem. 1971, 16, 103-220
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, vol.16
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Haddon, R.C.1
Haddon, V.R.2
Jackman, L.M.3
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68
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Trost, B. M.; Bright, G. M.; Frihart, C.; Brittelli, D. J. Am. Chem. Soc. 1971, 93, 737-745
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69
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80755181768
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This observation is re-enforced by Figure 3 of ref 61b, in which the bond currents in the 60 bonds of kekulene are expressed in terms of just three independent parameters, A, B, and δ. These are not actually the ring currents in the three symmetrically non-equivalent rings of kekulene, but they are related to them in the following way: the ring current in the six-membered ring that Steiner et al. (61b) label "I" is equal to (A + δ); the ring current in ring II is (A - δ), and that in the internal, 18-membered, ring III is (A - B). Once again, therefore, in this example, a bond-current description is entirely equivalent to a ring-current one, with as many independent variables being needed to specify the several bond currents as there are symmetrically non-equivalent rings (and, hence, distinct ring currents) in the structure under consideration
-
This observation is re-enforced by Figure 3 of ref 61b, in which the bond currents in the 60 bonds of kekulene are expressed in terms of just three independent parameters, A, B, and δ. These are not actually the ring currents in the three symmetrically non-equivalent rings of kekulene, but they are related to them in the following way: the ring current in the six-membered ring that Steiner et al. (61b) label "I" is equal to (A + δ); the ring current in ring II is (A - δ), and that in the internal, 18-membered, ring III is (A - B). Once again, therefore, in this example, a bond-current description is entirely equivalent to a ring-current one, with as many independent variables being needed to specify the several bond currents as there are symmetrically non-equivalent rings (and, hence, distinct ring currents) in the structure under consideration
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70
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0035820348
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Steiner, E.; Fowler, P. W.; Jenneskens, L. W.; Acocella, A. Chem. Commun. 2001, 659-660
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Chem. Commun.
, pp. 659-660
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Steiner, E.1
Fowler, P.W.2
Jenneskens, L.W.3
Acocella, A.4
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