132
S. Olsson et al. / Journal of Organometallic Chemistry 741-742 (2013) 131e135
obtained with high ee (89%). Bulk samples gave up to 71% ee
without optimisation of the crystallisation conditions. Di(indenyl)
zinc is best prepared by transmetallation of indenylpotassium with
C14
C13
zinc chloride in THF [9]. We found that a small excess of inden-
C15
1
ylpotassium facilitated the crystallisation of di(3-picoline)-di(1-
h
-
C16
C17
N2
C1
indenyl)zinc, and our manipulations with indenylpotassium led to
the accidental discovery of two indenylpotassium complexes
crystallising as conglomerates. Our investigations of these com-
plexes will be described in this paper.
C12
N3
N1
K1
C18
C11
C5
C10
C3
C4
C2
2
. Results and discussion
C9
C6
C8
2.1. Crystallisation
C7
Crystallisation of [K(ind)(pmdta)]
n
from benzene has been re-
-1, belong to the
ca. Like crystallisation from benzene, we
found that cooling a concentrated THF solution of [K(ind)(pmdta)]
invariably gave crystals of -1. (An excess of PMDTA was necessary,
ported previously [10], and the crystals obtained,
polar space group P2
a
1
n
a
however, to avoid precipitation of an unknown solid, presumably a
coordination polymer containing THF.) Upon cooling dilute solu-
Fig. 1. Molecular structure of b-1 displaying the crystallographic numbering scheme.
Displacement ellipsoids are drawn at the 50% probability level and all H atoms have
been omitted for clarity.
tions of [K(ind)(pmdta)]
space group P2 . We have not observed any indication of twinning-
by-inversion in -1 and crystallisation of -1 can therefore be
described as spontaneous resolution. In order to see whether -1
n
, a new phase (b-1) crystallised in Sohncke
1
shaped polymeric chains are centred on the 2
formationally chiral.
The same type of chains centred on 2
the main difference between the two structures is that adjacent
chains assume the same sense of chirality in -1, while -1 is
racemic. The calculated densities for -1 and -1 are similar: 1.134
1
-axes and are con-
b
b
b
1
-axes are found in a-1, and
had undergone total spontaneous resolution, two samples con-
sisting of relatively few crystals (which had formed slowly) were
examined, but enantiomorphic crystals were found within the
same sample. A well-known method in such cases is crystallisation
under slow stirring [11,12], but can be difficult to achieve at
depressed temperature over prolonged periods of time. In contrast
b
a
a
b
ꢀ
3
and 1.137 g cm , respectively. This indicates a similar packing ef-
ficiency [20], and explains the fact that the two phases may crys-
tallise concomitantly.
3 6 4 2
to e.g. the chiral reagents cis-[(p-CH C H )MgBr(dme) ] and cis-
The crystal structure of 2 displays the same type of polymeric
[
Mg(CH
3
)(thf)(dme)
2
]I, which crystallise as conglomerates at
ꢁ
chains as in
are separated by channels occupied by THF molecules (Fig. 2). As a
result, the structure is slightly less densely packed than -1 and -1,
a-1 and b-1, the largest difference being that the chains
ambient temperature and as racemic phases at ꢀ60 C [5], the
crystallisation of 1 does not appear to depend on the temperature,
a
b
since
b-1 has been obtained both at ambient temperature (by
ꢀ
3
ꢁ
ꢁ
the density being 1.128 g cm . The THF molecules form two CHeO
interactions with the PMDTA ligand, the O1eH18a and O1eH15b
layering the solution with n-hexane), at ꢀ30 C or at ꢀ80 C.
Following the method outlined in the experimental section, the
ꢀ
distances both being 2.66 A.
synthesis of
b-1 is perfectly reproducible. At intermediate con-
centrations, concomitant [13] crystallisation of the two phases was
observed. Concomitant crystallisation of racemates and conglom-
erates have attracted some attention [13,14], and we have observed
such phenomena for 10-nitro-phenantren-9-yl phenyl sulphide
2.3. Reactions with N-chlorosuccinimide
The crystal structure of
b
-1 is very different from that of di(3-
1
[
15], di(2,4-dimethylpyridino)-dichlorozinc [16] and di(3-picoline)-
picoline)-di(1-
nuclear molecules displaying indenyl anions bound in a
resulting in chirogenic -carbon atoms, while the polymeric
exhibits indenyl anions that are sandwiched between two K ions.
The two sides of the indenyl group in -1 are different; one side is
mode, while the opposite side is more
coordination. Investigation of the local
structure reveals that if the electrophile approaches an isolated
chain in -1, an ee would be obtained if the attack takes place
h -indenyl)zinc. The latter forms discrete mono-
1
1
di(1-
Cooling a very dilute solution to ꢀ80 C may initiate crystal-
lisation of the inclusion compound [K(ind)(pmdta)] (THF) (2), and
these crystals were found to belong to space group P2 . A Flack
h
-indenyl)zinc [8].
h
fashion,
-1
ꢁ
a
b
n
n
1
b
5
parameter [17e19] of ꢀ0.02(4) indicates that the analysed crystal
was enantiomerically pure, with no indication of twinning-by-
inversion. Of the two conglomerates, our efforts towards total
coordinated by a K ion in a h
3
accessible due to a
h
spontaneous resolution were concentrated on
b-1, which could be
b
obtained in the form of large single-crystals, while synthesis of 2
generally yields very small crystals. The synthesis of 2 is also
perfectly reproducible.
selectively on the less hindered side (Fig. 3).
When the complete crystal structure is examined, the difference
between the two sides of the indenyl anion is affected, since the
adjacent chains will fill up the space created in the grooves of the
zigzag chains. Nevertheless, it seemed to be worth trying to use
2.2. Crystal structures
crystals of b-1 in an asymmetric synthesis. Complex b-1 forms large
The three phases
the same type of polymeric chains. For example, each indenyl group
in -1 is coordinated by two K atoms exhibiting two different co-
ordination modes (Fig.1): K1 coordinates in a
other side of the indenyl plane, K1 (ꢀx, 1/2 þ y, ꢀz) coordinates in a
a
-1,
b
-1 and 2 are closely related and display
well-developed crystals, which make reactions on single-crystals
fairly simple. By performing reactions on single-crystals, one can
be sure to have an optically pure starting material. In the case of an
ee in a single-crystal reaction, reactions on bulk samples can be
performed; with knowledge of the ee obtained from a single-crystal,
b
5
h
-mode while, at the
3
h
-mode to C1, C8 and C9. Atom C8 is a part of the phenyl ring
one can get a rough estimate of the enantiomerical purity of the bulk
1
system rather than the cyclopentadienyl ring system. The zigzag
sample. During our investigations of di(3-picoline)-di(1-
h
-indenyl)