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85
2.9. Infrared spectroscopy
around all of the single bonds. The Monte Carlo calculations and
subsequent Rietveld refinements were repeated.
An infrared spectrum of each polymorphic form was recorded
using a JASCO FT/IR-420 instrument (JASCO International Co., Ltd.,
Tokyo, Japan) and the potassium bromide disk method.
3. Results and discussion
2
.10. 13C solid-state nuclear magnetic resonance spectroscopy
3.1. Polymorphic behavior
13C solid-state NMR spectra of the ␣-, -, and ␥-forms of ST
were measured using a Chemagnetics CMX Infinity 400 instrument
Chemagnetics, Fort Collins, CO, USA) operated at 100.3 MHz with a
We obtained four new forms of ST by recrystallizing ST and
seeding with ST-analogous compounds, and investigated their
physicochemical properties.
(
cross-polarization/magic angle spinning (CP/MAS) probe. CP/MAS
with two-pulse phase modulated (TPPM) decoupling was used, and
the sample was placed in a 4 mm outer diameter sample tube that
was rotated at 12 kHz. The contact time and the repetition time
were 5.0 ms, and 5.0 s, respectively. The spectral width was 40 kHz,
and 3000 scans were recorded.
Visual observations of all seven crystalline forms are shown
in Fig. 2. The crystalline forms had different morphologies. The
␣-Form crystals were massive and solid. The -, ␦-, and -Form
crystals were relatively large but fragile. The ␥- and -Form crystals
were fine, and the -form crystals were needles.
The PXRD patterns of the seven crystalline ST forms are shown in
Fig. 3. We confirmed that the ␣-, -, and ␦-form PXRD patterns coin-
cided with the patterns that were previously reported (Miura et al.,
2003; Takahashi et al., 2001; Ushio et al., 1996c, 2002). However,
the PXRD patterns of the four new crystals obtained in this study
were completely different from those of the other three forms, and
were also different from each other; each form showed a high
degree of crystallinity and distinct diffraction angles and inten-
sities. These results strongly suggested that the four new crystal
forms could be polymorphic forms of each other.
13C solid-state NMR spectra of the ␦-, -, -, and -forms of ST
were measured using a Chemagnetics CMX Infinity 400 instrument
(
Chemagnetics, Fort Collins, CO, USA), operated at 100.4 MHz, using
ramped CP/MAS with TPPM decoupling. The sample was placed in
a 5 mm outer diameter sample tube that was rotated at 10 kHz.
The contact time and the repetition time were 3.0 ms, and 5.0 s,
respectively. The spectral width was 40 kHz, and 400 scans were
recorded.
2
.11. Solubilities
Adding a small amount of an ST analogous compound to act as
seed crystals may have induced three of the new ST polymorphs
(␦-, -, and -forms) to crystallize. It is noteworthy that additives,
which made up less than 0.5% of the recrystallization solution in all
of the cases, caused new polymorphic forms to crystallize.
An excess amount of a polymorph sample was added to 2-
propanol (2 mL). The sample was vigorously shaken for 30 s every
5
◦
min for 30 min, and then allowed to stand for 4 h at 35.0 C.
The saturated solution was filtered through a 0.45 m mem-
brane filter, diluted with methanol, and analyzed by HPLC. HPLC
analyses were carried out using an octadecylsilanized silica gel
column (Shinwa chemical, ULTRON TDP, 4.6 mm × 150 mm), a mix-
ture of 2.5 mmol/L sodium 1-hexanesulfonate solution, acetonitrile,
and acetic acid (300:100:3) as the mobile phase at flow rate of
Kuroda et al. found a new polymorphic form of 6-
mercaptopurine, which was six to seven times more soluble
than the other known crystalline forms, by adding an analogous
compound as a seed (Kuroda et al., 1979). Kitamura and Ishizu
investigated the growth rate of l-glutamic acid in the presence of l-
phenylalanine, confirming that the polymorphic (␣- and -) forms
had different growth rates (Kitamura and Ishizu, 1998). Addadi
et al. successfully resolved d- and l-asparagine conglomerations
by adding small amounts of the pure enantiomers to saturated
solutions of d- and l-asparagine mixtures (Addadi et al., 1962).
It is thought that in each of these mechanisms, the analogous
compound adheres to a crystal surface and inhibits crystal growth.
In this study, it is considered that this mechanism also effects the
formation of new polymorphic forms of ST.
0.9 mL/min, and a UV–vis spectrophotometer (250 nm) as detector.
Powder X-ray diffraction was used to determine whether any of the
polymorphic forms had been transformed into another during the
solubility measurement process. The solubilities were determined
in duplicate.
2.12. Solving the crystal structures from the powder X-ray
diffraction data
Evaporating the chloroform from a supersaturated solution of
ST was an effective way of crystallizing the ␥-form, but the other
polymorphic forms were prepared by recrystallization.
The Reflex Plus module in the Materials Studio software (Accel-
rys, Inc, USA) was used for all calculations. The PXRD patterns of
the - and -form crystals of ST were indexed with the X-cell pro-
The DSC curves of the seven polymorphic forms of ST are shown
in Fig. 4. Each curve showed an endothermic peak due to fusion
◦
gram using 30 reflections (2ꢂ < 32 ). The cell and function profile
◦
parameters obtained were refined using the Pawley method. The
space group was determined from within the space group candi-
dates consistent with the systematic absences by a trial-and-error
method.
between 75 and 87 C.
◦
The highest melting points were 86.7 C for the ␣-form and
86.5 C for the ␥-form, showing that these polymorphic forms had
◦
spatially stable molecular arrangements. In contrast, low melting
points were observed for the ␦-, -, and -forms, indicating that
these forms were metastable. Furthermore, the polymorphic forms
prepared by pseudo-seeding with ST-analogous compounds (␦-,
-, and -forms) had broad endothermic peaks caused by melting-
point depression. The highest enthalpy of fusion was 39.9 kJ/mol
for the -form, and the lowest was 23.2 kJ/mol for the -form.
The IR spectra are shown in Fig. 5. For the known crystal struc-
tures (␣-, -, and ␦-forms), the carbonyl stretching band was found
Once the initial model molecular conformations of the - and
-form crystals of ST were assigned, the structures were solved
using the Monte Carlo/parallel tempering method in the Powder-
Solve software. Rietveld refinement was then performed, which
involved the following processes: (i) the pseudo Voight func-
tion was used to simulate the peak shape; (ii) the background
was determined by linear interpolation using 20 terms; (iii) the
Finger–Cox–Jephcoat method was used for asymmetric refine-
ment; and (iv) the March–Dollase method was applied to correct
preferred orientation effects. Global isotropic factors were used to
refine the temperature factors. The molecular conformation in each
of the motion groups was refined by varying the torsional angles
−
1
at 1664 cm
for the ␣-form (in which the carbonyl group was
hydrogen bonded to a OH group), whereas this band was shifted to
−
1
1678 and 1684 cm for the - and ␦-forms (in which the carbonyl
groups did not interact with a proton donor group).