Abstract
The edge strategy of Fujita’s unit-subduced-cycle-index (USCI) approach (S. Fujita,
“Symmetry and Combinatorial Enumeration in Chemistry,” Springer, 1991) is shown to be
effective for derivation based on a cubane skeleton, where twelve edges accommodate a set
of methano-bridges and/or ethano-bridges.
1 INTRODUCTION
Systematic derivation of high symmetry chiral molecules has been discussed qualitatively by
Farina and Morandi [1]. A more quantitative approach
based on mathematical foundations has been developed by Fujita under the name the
edge strategy (cf. Chapter 17 of [2]),
which is one embodiment of Fujita’s unit-subduced-cycle-index (USCI) approach [2]. The edge strategy has been applied to tetrahedrane of
Td-symmetry [3,4], cyclobutadiene of
D2d-symmetry [4], dodecahedrane of Ih -symmetry
[5], and fullerene of
Ih -symmetry [6].
The present article is devoted to the application of the edge strategy to a cubane skeleton
of Oh -symmetry, because cubane itself [7] and its derivatives such as basketane [8,9] and
D3 -trishomocubane [10,11,12] have attracted the interest of synthetic organic chemists, as summarized in a
review [13]. Although systematic discussions based on
D3-twisted bicyclo[2.2.2]octane molecular framework as a common
structural unit have appeared [14], the edge strategy
applied to a cubane skeleton aims at providing more quantitative perspectives.
2 THE EDGE STRATEGY APPLIED TOA CUBANE SKELETON
2.1 Theoretical Foundations
According to the edge strategy, an appropriate set of edges (bonds) selected from the
twelve edges (bonds) of a cubane skeleton 1 is replaced by a set of
m1 methano-bridges (solid circles) and
m2 ethano-bridges (pairs of solid circles), so as to give a
cage-shaped molecule. For example, a solid circle is placed to give 2, which
corresponds to the formation of homocubane 3 with a single methano-bridge, as
shown in Figure 1. The substitution of a pair of
solid circles produces 4, which corresponds to the formation of basketane
5 with a single ethano-bridge.
The cubane skeleton 1 belongs to the point group
Oh. Its 33 subgroups up to conjugacy
construct a non-redundant set of subgroups (SSG) [15]:
SSG
O
h
=
{
C
1
(
1
)
,
C
2
(
2
)
,
C
′
2
(
2
)
,
C
s
(
2
)
,
C
′
s
(
2
)
,
C
i
(
2
)
,
C
3
(
3
)
,
C
4
(
4
)
,
S
4
(
4
)
,
D
2
(
4
)
,
D
′
2
(
4
)
,
C
2
v
(
4
)
,
C
″
2
v
(
4
)
,
C
2
h
(
4
)
,
C
′
2
h
(
4
)
,
D
3
(
6
)
,
C
3
v
(
6
)
,
C
3
i
(
6
)
,
D
4
(
8
)
,
C
4
v
(
8
)
,
C
4
h
(
8
)
,
D
2
d
(
8
)
,
D
′
2
d
(
8
)
,
D
2
h
(
8
)
,
D
′
2
h
(
8
)
,
T
(
12
)
,
D
3
d
(
12
)
,
D
4
d
(
16
)
,
O
(
24
)
,
T
h
(
24
)
,
T
d
(
24
)
,
O
h
(
48
)
}
,
| (1) |
where the subgroups are aligned in the
ascending order of their orders, as listed in pairs of parentheses.
The twelve edges of the cubane skeleton 1 construct an orbit governed by the
coset representation
O
h
(
/
C
″
2
v
)
,
where the size of the orbit is equal to the degree of the
coset representation, i.e.,
|
O
h
|
/
|
C
″
2
v
|
=
48
/
4
=
12.
2.2 The Fixed-Point-Matrix (FPM) Method of Fujita’s USCI Approach
Fujita’s USCI approach supports four methods of symmetry-itemized enumeration [2]. Among them, the present article applies the
fixed-point-matrix (FPM) method to count cubane derivatives. It is because the FPM method
gives results in succinct tabular forms, while the other methods provide equivalent
results in more complex forms (e.g., in the form of generating functions). A set of unit
subduced cycle indices with chirality fittingness (USCI-CFs) for the
O
h
(
/
C
″
2
v
)
-orbit is cited from Tables 4 and 5 of [16] as follows:
(
b
1
12
,
b
2
6
,
b
1
2
b
2
5
,
a
1
4
c
2
4
,
a
1
2
c
2
5
,
c
2
6
,
b
3
4
,
b
4
3
,
c
4
3
,
b
4
3
,
b
2
2
b
4
2
,
a
2
4
c
4
,
a
2
2
c
4
2
,
a
1
2
a
2
c
4
2
,
a
2
2
c
4
2
,
a
2
c
2
c
4
2
,
b
3
2
b
6
,
a
3
2
c
6
,
c
6
2
,
b
4
b
8
,
a
4
3
,
a
4
c
8
,
a
4
c
8
,
a
4
2
c
4
,
a
4
3
,
a
2
2
c
8
,
b
12
,
a
6
c
6
,
a
4
a
8
,
b
12
,
a
12
,
a
12
,
a
12
)
,
| (2) |
where the USCI-CFs are aligned in accord
with the SSG (Eq. 1).
Suppose that each edge is substituted by a methano-bridge, an ethano-bridge, or a null
unit (no substitution). Dummy variables x, y, and
z are respectively used for null units (no substitution),
for methano-brides, and for ethano-bridges. Then, a single inventory function is used as follows:
a
d
=
b
d
=
c
d
=
x
d
+
y
d
+
z
d
.
| (3) |
The inventory function (Eq. 3) is introduced into the USCI-CF of each subgroup listed in
equation. 2. The resulting equation is expanded to give a generating function for the
subgroup at issue, where the coefficient of each term
x
m
0
y
m
1
z
m
2
represents the number of fixed derivatives with
m0 null units (no substitution),
m1 methano-bridges (solid circles), and
m2 ethano-bridges (pairs of solid circles), where
m0+m1+m2
= 12. A fixed-point vector (FPV) is obtained by aligning the coefficients of
x
m
0
y
m
1
z
m
2
in the order of the SSG (Eq. 1). Then, the corresponding
fixed-point matrix (FPM) is obtained by moving m0,
m1, and m2 to satisfy
m0+m1+m2
= 12, where the FPV for
x
m
0
y
m
1
z
m
2
appears as a row vector of the FPM.
The resulting FPM is multiplied by the inverse mark table
M
O
h
−
1
(e.g., Table 2 of [16]) to give an isomer-counting matrix (ICM):
ICM
=
FPM
×
M
O
h
−
1
,
| (4) |
where each row shows the numbers of
cage-shaped derivatives with
x
m
0
y
m
1
z
m
2
in the alignment of the SSG (Eq. 1). The procedure for
calculating the ICM has been programmed by means of the Maple system in a similar way to
the source code described in [
16].

Table 1.
Symmetry-Itemized Numbers of Cage-Shaped Molecules (Part I)

Table 2.
Symmetry-Itemized Numbers of Cage-Shaped Molecules (Part II)
Because the term
x
m
0
y
m
1
z
m
2
appears symmetrically in the generating function, the
partition [m0, m1,
m2] (m0 ≥
m1 ≥ m2) is used to represent
terms
x
m
0
y
m
1
z
m
2
,
x
m
0
y
m
2
z
m
1
,
x
m
1
y
m
0
z
m
2
,
x
m
1
y
m
2
z
m
0
,
and so on.
The ICM of the partition [m0, m1,
0] is shown in Table 1, where each row
contains the symmetry-itemized values in the alignment of SSG (Eq. 1). The partition
[m0, m1, 0] (corresponding to
x
m
0
y
m
1
or
x
m
0
z
m
2
) means the single substitution of methano-bridges (or
ethano-bridges) on edges. Each value of Table
1 represents the number of pairs of (self-) enantiomers, where a pair of
self-enantiomers means an achiral derivative. Note that the values for [11,0,1] are equal
to the values collected in the [11,1,0] -row; the values for [5,7,0] (or for [5,0,7]) are
equal to the values collected in the [7,5,0]-row; and so on.
Table 2 collects symmetry-itemized numbers of
cage-shaped molecules, each of which exhibits mixed appearance of
m1 methano-bridges (m1 > 0)
and m2 ethano-bridges (m2 >
0).
3 CAGE-SHAPED MOLECULES DERIVED BYTHE EDGE STRATEGY
3.1 Cage-Shaped Molecules with Either Methano- or Ethano-Bridges
Table 1 summarizes the symmetry-itemized
enumeration of cage-shaped molecules with methano- or ethano-bridges.
The value 1 at the intersection between the [12,0,0]-row and the
Oh-column (the 33rd column) in Table 1 indicates the existence of one
Oh-molecule, which corresponds to cubane
1 itself, dodecakismethanocubane ([0,12,0]), or dodecakisethanocubane
([0,0,12]).
The [11,1,0]-row of Table 1 (at the
14th-column) indicates that there appears one
C
″
2
v
-molecule, which corresponds to a cage-shaped molecule with
one methano-bridge 2 (homocubane 3) or a cage-shaped molecule
with one ethano-bridge 4 (bascketane 5, strictly speaking
[11,0,1]), as depicted in Figure 1.
The [10,2,0]-row of Table 1 indicates that
there are one pair of enantiomeric
C
′
2
-molecules, one
C
′
s
-molecule, one
C2v-molecule, and one
D
′
2
h
-molecule. These bismethanocubanes are depicted in Figure 2.
The
C
′
2
-molecule 6(or its enantiomer
6
¯
), which is called C2-bishomocubane,
possesses a two-fold rotation axis running through the midpoints of the edges 2–6 and 4–8.
Synthesis and absolute configuration of optically active
C2-bishomocubane
6
¯
have been reported [17]. The
C
′
s
-molecule 7 possesses a mirror plane containing
vertices 2, 4, 8, 6. The C2v-molecule
8 possesses a two-fold axis running through the centers of the top and
bottom faces. The
D
′
2
h
-molecule 9 possesses a vertical two-fold axis
running through the centers of the top and bottom faces as well as two two-fold axes
perpendicular to the vertical axis.
The [9,3,0]-row of Table 1 indicates that
there are two pairs of enantiomeric C1-molecules (
1
0
/
1
0
¯
and
1
1
/
1
1
¯
), one pair of enantiomeric
C
′
2
-molecules (
1
2
/
1
2
¯
), two Cs-molecules
(13 and 14), one
C
′
s
-molecule (15), one
C
″
2
v
-molecule (16), one pair of enantiomeric
D3-molecules (
1
7
/
1
7
¯
), and one
C3v-molecule (18).
These trismethanocubanes are depicted in Figure
3.
The two-fold axis of the
C
′
2
-molecule 12 (or
1
2
¯
) runs through the midpoints of edges 1–6 and 4–8. The
mirror plane of the Cs-molecule 13
(or 14) is perpendicular to the front and back faces and bisects the
cube vertically. The mirror plane of the
C
′
s
-molecule 15 is contained in the plane 2–6–4–8.
The two-fold axis of the
C
″
2
v
-molecule 16 runs through the midpoints of the
edges 2–6 and 4–8. The three-fold axis of the D3-molecule 17
(or
1
7
¯
) runs through the vertices 6 and 4. The three-fold axis of
the C3v-molecule 18 runs
through the vertices 6 and 4.
Among the trismethanocubanes depicted in Figure
3, the D3-molecule 17 or
1
7
¯
is called D3-trishomocubane. The
syntheses of
1
7
/
1
7
¯
have been reported by Underwood [18] and by Kent et al. [10]. The
absolute configuration of (−)D3-trishomocubane 17 has
been determined by Helmchen and Staiger [11], while
the absolute configuration of (+)D3-trishomocubane
1
7
¯
has been determined by Nakazaki et al. [12].
3.2 Cage-Shaped Molecules with Both Methano- and Ethano-Bridges
Let us examine the
C
″
2
v
-column (the 14th column) of Table 2. The value of each row shows the number of cage-shaped
molecules, as collected in Figure 4.
For the purpose of depicting cage-shaped molecules of
C
″
2
v
-symmetry, we presume that the two-fold axis of
C
″
2
v
runs through the midpoints of the edges of 2–6 and 4–8.
According to Fujita’s USCI approach [2], the
derivation of such
C
″
2
v
-molecules is controlled by the following subduction:
O
h
(
/
C
″
2
v
)
↓
C
″
2
v
=
2
C
″
2
v
(
/
C
1
)
+
C
″
2
v
(
/
C
s
)
+
2
C
″
2
v
(
/
C
″
2
v
)
.
| (5) |
This subduction corresponds to the USCI-CF
a
1
2
a
2
c
4
2
, which appears as the 14th element of equation. 2.
The twelve edges of a
C
″
2
v
-molecule are divided into the following orbits:
{
2
−
6
}
Δ
1
C
″
2
v
(
/
C
″
2
v
)
| (6) |
{
4
−
8
}
Δ
2
C
″
2
v
(
/
C
″
2
v
)
| (7) |
{
1
−
5
,
3
−
7
}
Δ
3
C
″
2
v
(
/
C
s
)
| (8) |
{
1
−
2
,
2
−
3
,
5
−
6
,
6
−
7
}
Δ
4
C
″
2
v
(
/
C
1
)
| (9) |
{
1
−
4
,
3
−
4
,
5
−
8
,
7
−
8
}
Δ
5
C
″
2
v
(
/
C
1
)
| (10) |
Each orbit accommodates methano-bridges (or ethano-bridges) in accord with its size.
For example, one
C
″
2
v
-molecule 19, which corresponds to the value
appearing at the intersection between the [10,1,1]-row and the
C
″
2
v
-column (the 14th column) of Table 2, is depicted by placing an ethano-bridge on the orbit
Δ1, a methano-bridge on the orbit Δ2, and null units on the
remaining orbits Δ3, Δ4, and Δ5.
The derivation of 26 and 27 illustrates two different modes of
packing of ethano-bridges. Two ethano-bridges separately occupy two one-membered orbits
Δ1 and Δ2 in 26, so that they are inequivalent to
each other. On the other hand, two ethano-bridges occupy a two-membered orbit
Δ3 of 27, so that they are equivalent to each other.
CONCLUSION
The edge strategy proposed in Chapter 17 of [2] is
effective for derivation based on a cubane skeleton, where twelve edges accommodate a set of
methano-bridges and/or ethano-bridges. The fixed-point-matrix (FPM) method of Fujita’s USCI
approach is applied to symmetry-itemized enumeration of cage-shaped molecules by starting
from the cubane skeleton of Oh.
References
- [1] M. Farina, C. Morandi,
Tetrahedron, 30, 1819 (1974).
- [2] S. Fujita, “Symmetry and
Combinatorial Enumeration in Chemistry”, Springer-Verlag, Berlin-Heidelberg
(1991).
- [3] S. Fujita, Bull. Chem. Soc.
Jpn., 62, 3771 (1989).
- [4] S. Fujita, Tetrahedron, 46,
365 (1990).
- [5] S. Fujita, Bull. Chem. Soc.
Jpn., 63, 2759 (1990).
- [6] S. Fujita, J. Chem. Inf.
Comput. Sci., 36, 270 (1996).
- [7] P. E. Eaton, T. W. Cole, J.
Am. Chem. Soc., 86, 3157 (1964).
- [8] S. Masamune, H. Cuts, M. G.
Hogben, Tetrahedron Lett., 7, 1017 (1966).
- [9] W. G. Dauben, D. L. Whalen,
Tetrahedron Lett., 7, 3743 (1966).
- [10] G. J. Kent, S. A. Godleski,
E. Osawa, and P. von R. Schleyer, J. Am. Chem. Soc., 42, 3852–3859
(1977).
- [11] G. Helmchen, G. Staiger,
Angew. Chem. Int. Ed. Engl., 16, 116 (1977).
- [12] M. Nakazaki, K. Naemura, N.
Arashiba, J. Org. Chem., 43, 689 (1978).
- [13] A. P. Marchand, Chem. Rev.,
89, 1011 (1989).
- [14] M. Nakazaki, K. Naemura,
Yuki Gosei Kagaku Kyokai-Shi, 40, 1128 (1982).
- [15] S. Fujita, Polyhedron, 12,
95 (1993).
- [16] S. Fujita, Bull. Chem. Soc.
Jpn., 84, 1192 (2011).
- [17] M. Nakazaki, K. Naemura, J.
Org. Chem., 42, 2985 (1977).
- [18] G. R. Underwood, B.
Ramamoorthy, Tetrahedron Lett., 11, 4125 (1970).