Interaction between the Pyrimidic Nucleotides 5’-CMP, 5’-dCMP, and 5’-UMP and Diethyltin Dichloride
35Cl chemical shifts were referenced to a solution of NaCl (1 ,
mass spectra, and Prof. Dr. Ir. B. Van Mele and Dr. Ir. H. Rahier
FULL PAPER
δ ϭ 0). The 15N chemical shifts were referenced to Ξ ϭ for access to the IR, Raman and thermogravimetric analysis facilit-
10.136767 MHz.[46b]
ies. J. C. M. is a postdoctoral research associate of the Fund for
Scientific Research Flanders (Belgium). The financial support by
the ‘‘Bourse de la Fondation David et Alice Van Buuren’’ (L. G.),
the Belgian ‘‘Fonds voor Kollektief Fundamenteel Onderzoek’’
(FKFO Grant N° 2.0094.94, R. W., M. B.), the Belgian ‘‘Nationale
Loterij’’ (Grants N° 9.0006.93 and 9.0192.98, R. W., M. B.), the
Fund for Scientific Research Flanders (Belgium, Grant N°
G.0192.98, R. W, M. B.), and the Belgian ‘‘Nationaal Fonds voor
Wetenschappelijk Onderzoek’’ (NFWO Grant N° G.0054.96, M.
G.) is gratefully acknowledged.
Broad band 1H-decoupled 13C and 119Sn spectra were recorded us-
ing the Bruker pulse sequences with standard delays. The 1D and
1
2D H-119Sn HMQC experiments consisted of gradient enhanced-
versions of the standard HMQC pulse sequence processed in the
magnitude mode and implemented as described elsewhere.[32] The
2D 31P-1H HOESY[16,17] experiments were performed by recording
128 FIDs of 1 K data points, 144 scans each, with an acquisition
time of 0.2 s, a relaxation delay of 1.6 s and a mixing time of 1 s.
The 2D 1H-15N HMQC spectra were typically obtained by record-
ing 64 FIDs of 4 K data points, 32 scans each, with an acquisition
time of 0.5 s and a relaxation delay of 1.5 s. The 2D 119Sn EXSY
spectra were typically obtained by recording 24 FIDs of 4 K data
points, 3,200 scans each, with an acquisition time of 0.1 s, a relaxa-
tion delay of 1 s and a mixing time of 10 ms.
[1]
B. K. Keppler, Metal Complexes in Cancer Chemotherapy,
VCH, Weinheim, 1993.
[2]
A. T. M. Marcelis, J. Reedijk, Recl. Trav. Chim. Pays-Bas 1983,
102, 121–129.
[3]
S. J. Lippard, Science 1982, 218, 1075–1082.
[4]
M. Bloemink, J. Reedijk, Metal Ions in Biology (Eds.: A. Sigel,
All CP-MAS NMR spectra[47] were recorded on a Bruker AC250
and, in later stages, on a Bruker DRX250 spectrometer operating
at 101.26, 62.90, and 89.15 MHz for 31P, 13C, and 117Sn nuclei,
respectively. The spectrometer was equipped with a 7 or 4 mm
MAS broad-band probe. The matching conditions for Hartmann-
Hahn cross-polarization[47] (pulse length 5 µs) and the chemical
shift reference for the 117Sn nucleus were set with (cyclo-C6H11)4Sn
[δ ϭ–97.35 relative to (CH3)4Sn]. The 13C chemical shift reference
frequency was set with adamantane. The 117Sn spectra were typic-
ally obtained by acquiring 32 K data points over a spectral width
of 166.7 kHz, a 2 ms contact time and a relaxation delay of 2 s
with 10,000 to 20,000 scans. The isotropic chemical shifts were
identified by recording two spectra with sufficiently different spin-
ning rates.[47] The 13C CP-MAS spectra were obtained by acquiring
4 K data points over a spectral width of 17 kHz, a 2 ms contact
time and a relaxation delay of 4 s with 1,000 to 10,000 scans. The
1H-decoupled 31P MAS spectra were obtained by acquiring 4 K
data points over a spectral width of 20 kHz and a relaxation delay
of 4 s with 100 to 1,000 scans.
H. Sigel), M. Dekker, New-York 1996, 32, p. 641.
[5]
T. D. Tullius, S. J. Lippard, J. Am. Chem. Soc. 1981, 103,
4620–4622.
[6]
M. Gielen, Coord. Chem. Rev. 1996, 151, 41–51.
[7]
A. J. Crowe, Drugs of the Future 1987, 12, 255–275.
[8]
R. Barbieri, A. Silvestri, J. Inorg. Biochem. 1991, 41, 31–35.
[9]
V. Piro, F. Di Simone, G. Madonia, A. Silvestri, A. M. Giuli-
ani, G. Ruisi, R. Barbieri, Appl. Organomet. Chem. 1992, 6,
537–542.
[10]
R. Barbieri, A. Silvestri, A. M. Giuliani, V. Piro, F. Di Simone,
G. Madonia, J. Chem. Soc., Dalton Trans. 1992, 585–590.
[11] [11a] Q. Li, P. Yang, H. Wang, M. Guo, J. Inorg. Biochem. 1996,
[11b]
64, 181–195. –
Z. Yang, T. Bakas, A. Sanchez-Diaz, C.
Charalambopoulos, J. Tsangaris, N. Hadjiliadis, J. Inorg. Bi-
[11c]
ochem. 1998, 72, 133–140. –
A. Jancso, L. Nagy, E. Mol-
drheim, E. Sletten, J. Chem. Soc., Dalton Trans. 1999, 1587–
1594.
[12]
[13]
[14]
[15]
D. P. Bancroft, C. A. Lepre, S. J. Lippard, J. Am. Chem. Soc.
1990, 112, 6860–6871.
F. Kayser, M. Biesemans, M. Gielen, R. Willem, J. Magn. Re-
son. 1993, A102, 249–252.
J. C. Martins, P. Verheyden, F. Kayser, M. Gielen, R. Willem,
M. Biesemans, J. Magn. Reson. 1997, 124, 218–222.
F. Kayser, M. Biesemans, M. Gielen, R. Willem, Advanced Ap-
plications of NMR to Organometallic Chemistry (Eds.: M. Gi-
elen, R. Willem, B. Wrackmeyer), Wiley, Chichester, 1996,
chapter 3, 45–86.
C. Yu, G. C. Levy, J. Am. Chem. Soc. 1983, 105, 6994–6996.
C. Yu, G. C. Levy, J. Am. Chem. Soc. 1984, 106, 6533–6537.
F. Ribot, C. Sanchez, R. Willem, J. C. Martins, M. Biesemans,
Inorg. Chem. 1998, 37, 911–917.
K. C. Molloy, Chemistry of tin (Ed.: P. J. Smith), Blackie Aca-
demic Professional, Thomson Science, London, 1998, 2nd edi-
tion, p. 138.
R. C. Poller, J. Organomet. Chem. 1965, 3, 321–329.
A. G. Davies, Organotin Chemistry, VCH, Weinheim, 1997, p.
144.
Infrared Spectroscopy: Infrared spectra were acquired from KBr
pellets in the Fourier transform mode from a Perkin–Elmer System
2000 FT-IR spectrometer. The Raman spectra were acquired in the
Fourier-transform mode from a Perkin–Elmer System 2000 NIR
FT-RAMAN spectrometer using a Raman dpy2 beam with
310 mW power.
[16]
[17]
[18]
Electrospray Mass Spectrometry: The electrospray mass spectra
were recorded in the cationic and anionic modes on a Micromass
Quattro II instrument coupled to a Masslynx system (ionisation in
an electric field of 3.5 kV; source temperature 80 °C; source pres-
sure 1 atm.; analyser pressure 10–5 mbar).[48] Cone voltages were
15 V. Calculated and experimental isotopic distributions were com-
pared using the shareware program MassCluster v.2.1. for Apple
Macintosh. The m/z ratios reported in Table 1 and Figure 3 corre-
spond to the peak with the highest intensity of the isotopic distri-
bution patterns.
[19]
[20]
[21]
[22] [22a]
D. Dakternieks, K. Jurkschat, S. van Dreumel, E. R. T.
[22b]
Tiekink, Inorg. Chem. 1997, 36, 2023–2029. –
T. Yano, K.
Nakashima, J. Otera, R. Okawara, Organometallics 1985, 4,
1501–1503.
[23] [23a]
A. Bax, M. F. Summers, J. Magn. Reson. 1986, 67, 565–
[23b]
569. –
A. Bax, R. H. Griffey, B. L. Hawkins, J. Magn.
Reson. 1983, 55, 301–315.
A. Bax, M. F. Summers, J. Am. Chem. Soc. 1986, 108, 2093–
Thermogravimetric Analysis: The thermogravimetric analysis was
made on a Perkin–Elmer TGA-7 thermogravimetric analyser by
heating the sample from 40 to 500 °C at 10 °C/min under a nitro-
gen atmosphere.
[24]
[25]
2094.
ˆ
F. Kayser, M. Biesemans, M. Boualam, E. R. T. Tiekink, A. El
Khloufi, J. Meunier-Piret, A. Bouhdid, K. Jurkschat, M. Gi-
elen, R. Willem, Organometallics 1994, 13, 1098–1113; 4126
K. J. Barnham, C. J. Bauer, M. I. Djuran, M. A. Mazid, T.
Rau, P. J. Sadler, Inorg. Chem. 1995, 34, 2826–2832.
D. Neuhaus, M. Williamson, The Nuclear Overhauser Effect in
Structural and Conformational Ananlysis, VCH Publishers,
New-York, 1984.
[26]
[27]
Acknowledgments
We thank Mrs I. Verbruggen for recording some of the NMR spec-
tra, Dr. G. Laus and Mr. M. Desmet for recording the electrospray
Eur. J. Inorg. Chem. 2000, 513Ϫ522
521