K Fukui
21
Fig. 5. A comparison of HOMO and the interaction frontier orbital for protonation in styrene.
FRONTIER ORBITALS IN RELATED FIELDS
Theoretical treatments of the property of solid crystals, or chemisorption on a
solid surface, appear to have hitherto been almost monopolistically treated by
the methodology of physics. But the orbital pattern technique has also ad-
vanced gradually in this field.
The “cluster approach, ”
81, 82
in which a portion of the metal crystal is
drawn out as the form of a cluster of atoms and its catalytic actions or other
properties are investigated, has contributed to the development of the orbital
pattern approach, because the physical methods mentioned above can hardly
be applied to such sizable systems. It is expected that, if clusters of various sizes
and various shapes are studied to look into the characteristic feature of their
HOMO’s (high-lying occupied MO’s) and LUMO’s (low-lying unoccupied
MO’s), the nature of chemisorption and catalytic action, the mode of surface
chemical reaction, and several related subjects of interest can be investigated
theoretically.
As is the case of molecular interactions in usual chemical reactions, only the
HOMO- and LUMO-bands lying in the range of several electron volts near the
Fermi level can participate in the adsorption of molecules and surface reactions
on solid crystals. You may recollect here that, in the BCS (Bardeen-Cooper-
Schrieffer) theory of superconductivity, too, only the HOMO’s and LUMO’s
in close proximity to the Fermi surface can be concerned in forming electron
pairs as the result of interaction with lattice vibration. In the case of solid
catalysts mentioned above, the discrimination of particular orbitals and elec-
trons from the others have made the situation much easier.
Consider a system composed of a regular repetition of a molecular unit, for
instance, a one-dimensional high polymer chain or a one-dimensional lattice, in
which a certain perturbation is imposed at a definite location. Sometimes it is
convenient to discuss the influence of this perturbation by transforming the
22
Chemistry 1981
orbitals belonging to the HOMO-band to construct the orbitals localized at
that place. One such technique was proposed by Tanaka, Yamabe and my-
self.
83
This method is expected to be in principle applied to a local discussion
of such problems as the adsorption of a molecule on the two-dimensional
surface of catalysts, surface reactions, and related matters. This approach may
be called a little more chemical than the method using the function of local
density of states
84
or similar ones, in that the former can be used for the
argument of the reactivity of molecules on a catalyst surface in terms of the
phase relationship of localized orbitals.
What is called low-dimensional semiconductors and some superconductors
have also been the objects of application of the orbital argument. In these
studies, the dimerization of S
2
N
2
to S
4
N
4
85
and the high-polymerization to
( S N )
x
8 6
were discussed, and the energy band structure of (SN)
x
polymer chain
was analyzed to investigate the stable nuclear arrangement and the mode of
inter-chain interactions.
87
The modern technique employed in solid state physics to interpret the
interesting characteristic behaviours of noncrystalline materials, in particular
of amorphous materials, in which the nuclear arrangements were not regular,
was certainly striking. Anderson showed generally that in a system of random
lattice the electron localization should take place.
56
Mott, stating in his 1977
Nobel lecture that he thought is the first prize awarded for the study of
amorphous materials, answered the question, “How can a localized electron be
conducted?” with the use of the idea of hopping. Here, too, the HOMO-
LUMO interaction - in this case the consideration of spin is essential - would
play an important part.
Here in a few words, I want to refer to the meaning and the role of virtual
orbitals. The LUMO, which has been one of the stars in orbital arguments
hitherto discussed, is the virtual orbital which an external electron is consid-
ered to occupy to be captured by a molecule to form an anion. Virtual orbitals
always play an essential part in producing metastable states of molecules by
electron capture.
88
To discuss such problems generally, Tachibana et al.
89
systematized the theory of resonant states from the standpoint of complex
eigenvalue problem. The idea of resonant states will take a principal part in
chemical reactions, particularly in high-energy reactions which will be devel-
oped more in the future.
PROSPECT
In introducing above a series of recent results of the studies carried out mainly
by our group, I have ventured to make those things the object of my talk which
are no more than my prospective insight and are not yet completely estab-
lished. This is just to stimulate, by specifying what are the fields I believe
promising in the future, the intentional efforts of many younger chemists in
order to develop them further.
In my opinion, quantum mechanics has two different ways of making partici-
pations in chemistry. One is the contribution to the nonempirical comprehen-
K. Fukui
23
sion of empirical chemical results just mentioned. However, we should not
overlook another important aspect of quantum mechanics in chemistry. That is
the promotion of empirical chemistry from the theoretical side. But, also for
this second purpose, as a matter of course, reliable theoretical foundations and
computational methods are required. The conclusions of theories should be
little affected by the degree of sophistication in approximations adopted.
On the other hand, for theoreticians to make the second contribution, the
cases where predictions surpassing the experimental accuracy are possible by
very accurate calculations are for the present limited to those of a very few,
extremely simple molecules. In order to accomplish this object in regard to
ordinary chemical problems, it becomes sometimes necessary to provide quali-
tative theories which can be used even by experimental chemists. If one can
contribute nothing to chemistry without carrying out accurate calculations
with respect to each problem, one can not be said to be making the most of
quantum mechanics for the development of chemistry. It is certainly best that
the underlying concepts are as close to experience as possible, but the sphere of
chemical experience is steadily expanding. Quantum chemistry has then to
perform its duty by furnishing those concepts with the theoretical basis in order
to make them chemically available and serviceable for the aim of promoting
empirical chemistry.
Even the same atoms of the same element, when they exist in different
molecules, exhibit different behaviours. The chemical symbol H even seems to
signify atoms of a completely different nature. In chemistry, this terrible
individuality should never be avoided by “averaging,” and, moreover, innu-
merable combinations of such atoms form the subject of chemical research,
where it is not the “whole assembly of compounds of different kinds but each
individual kind of compounds” that is of chemical interest. On account of this
formidable complexity, chemistry possesses inevitably one aspect of depending
on the analogy through experience. This is in a sense said to be the fate alloted
to chemistry, and the source of a great difference in character from physics.
Quantum chemistry, too, so far as it is chemistry, is required to be useful in
promoting empirical chemistry as mentioned before.
ACKNOWLEDGEMENTS
Lastly, I want to mention at this opportunity out of a sense of gratefulness the
names of many people in our group who have been walking on the same road as
mine since my first paper (1952) on quantum chemistry, particularly Drs. T.
Yonezawa, C. Nagata, H. Kato, A. Imamura, K. Morokuma, T. Yamabe and
H. Fujimoto, and also I can not forget the names of younger doctors mentioned
in the text who made a contribution in opening new circumstances in each
field. Among them, Prof. T. Yonezawa was helpful in performing calculations
in our 1952 paper, and also, it is to be mentioned with appreciation that the
attractive title “frontier orbitals” of my lecture originated from the terminology
I adopted in that paper by the suggestion of Prof. H. Shingu, who kindly
participated in that paper as an organic chemist to classify the relevant experi-
24
Chemistry 1981
mental results. Furthermore, many other collaborators are now distinguishing
themselves in other important fields of chemistry, which, however, have not
been the object of the present lecture.
It was the late Prof. Yoshio Tanaka of the University of Tokyo and Prof.
Masao Horio of Kyoto University who recognized the existence and signifi-
cance of my early work in advance to others. I owe such a theoretical work,
which I was able to carry out in the Faculty of Engineering, Kyoto University,
and moreover in the Department of Fuel Chemistry, to the encouragement and
kind regard of Prof. Shinjiro Kodama, who fostered the Department. What is
more, it was the late Prof. Gen-itsu Kita, my life-teacher, and the founder of the
Department, who made me enter into chemistry, one of the most attractive and
promising fields of science, and led me to devote my whole life to it. For all of
these people no words of gratitude can by any means be sufficient.
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K. Fukui
25
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26
Chemistry 1981
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