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Fig. 4 Motifs found in the 1:1 cocrystals of (a) 1-DAP as the stable 3H tautomer with I2 and I1 and (b) 1-DAP as the metastable 1H tautomer with U3, U13, U4 and U1.
Table 1 Dimer energies (kJ molꢀ1) between one molecule of 1-DAP and its two
contribution may prove very useful for the design of new
materials containing rare tautomeric forms, which are likely
closest neighbours in four relevant cocrystals
to exhibit very different physical properties. This should be of
Dimer interacting through
interest to many research areas dealing with the solid-state
Two hydrogen bonds
(3H–3H)
One halogen bond
(3H–I)
properties of high-value active ingredients and materials.
AJCC acknowledges the Netherlands Organization for Scientific
Research for a VENI grant.
Cocrystal
3H:I1
3H:I2
ꢀ96.5
ꢀ98.1
ꢀ36.5
ꢀ37.9
Two hydrogen bonds
(1H–U)
One hydrogen bond
(1H–U)
Notes and references
‡ This structure was later found to correspond to the crystal structure
observed experimentally.20
1H:U1
1H:U13
ꢀ74.0
ꢀ86.1
ꢀ48.3
ꢀ47.3
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Inc., San Diego, 2000, vol, 76, pp. 1–84.
To understand the overall stabilities of the systems, one
needs to compare the lattice energies of the cocrystal structures
with respect to the lattice energies of the single component
crystal structures.17–19 Lattice energies for the cocrystals 3H:I2
and 1H:U1 and the coformers I2 and U1 were calculated by
geometry optimizing the experimentally known crystal struc-
tures with VASP (PBE-d). The lattice energy of pure 1-DAP was
taken from the most stable crystal structure generated compu-
tationally and energy minimized using the same method.‡
The cocrystallization energy was calculated as the difference
between the lattice energy of the cocrystal and those of the
4 J. Elguero, Struct. Chem., 2012, 23, 297–300.
5 A. J. Cruz-Cabeza and C. R. Groom, CrystEngComm, 2011, 13, 93.
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8 M. U. Schmidt, J. Bruening, J. Glinnemann, M. W. Huetzler,
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single component crystal structures. For both cocrystals 3H:I2 10 M. Tutughamiarso and E. Egert, Acta Crystallogr., Sect. B, 2012, 68,
444–452.
and 1H:U1, the cocrystallization energy was found to be negative,
¨
11 C. B. Aakeroy, A. M. Beatty and B. A. Helfrich, Angew. Chem., Int. Ed.,
ꢀ9 and ꢀ6 kJ molꢀ1 respectively. A negative cocrystallization
2001, 40, 3240–3242.
energy indicates that cocrystal formation is driven by an 12 G. R. Desiraju, Angew. Chem., Int. Ed., 2007, 46, 8342–8356.
13 P. G. Karamertzanis and C. C. Pantelides, J. Comput. Chem., 2005,
enthalpic gain. The energy gain afforded through the formation
26, 304–324.
of the 1H:U1 cocrystal, however, is less stabilizing (ꢀ6 kJ molꢀ1
)
14 G. Kresse and J. Hafner, Phys. Rev. B, 1993, 47, 558; G. Kresse and
J. Hafner, Phys. Rev. B, 1994, 49, 14251; G. Kresse and J. Furthmu¨ller,
Comput. Mater. Sci., 1996, 6, 15–50.
15 J. P. Perdew, K. Burke and M. Ernzerhof, Phys. Rev. Lett., 1996, 77,
3865–3868.
than the energy gain afforded through the formation of the
3H:I2 cocrystal (ꢀ9 kJ molꢀ1), perhaps, amongst other contri-
butions, because of the higher tautomeric energy of the former.
In summary, we have been able to extract desired molecular 16 S. Grimme, J. Comput. Chem., 2006, 27, 1787–1799.
17 A. J. Cruz-Cabeza, G. M. Day and W. Jones, Chem.–Eur. J., 2008, 14,
tautomers into the solid state using supramolecular selectivity
driven by both hydrogen and halogen bond based interactions.
This study illustrates how relative stabilities of tautomers can
drastically change with a change of environment and how, by
controlling the environment, it is possible to deliberately
isolate a desired tautomer. The concepts illustrated in this
8830–8836.
´
´
ˇˇ ´
18 A. J. Cruz-Cabeza, S. Karki, L. Fabian, T. Friscic, G. M. Day and
W. Jones, Chem. Commun., 2010, 46, 2224–2226.
19 H. C. S. Chan, J. Kendrick, M. A. Neumann and F. J. J. Leusen,
CrystEngComm, 2013, 15, 3799–3807.
´
´
20 L. Dyminska, A. Gagor, M. Maczka, Z. Weglinski and J. Hanuza,
J. Raman Spectrosc., 2010, 41, 1021–1029.
c
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