Angewandte
Chemie
(d, J = 8.6 Hz, 4H, thread ArH), 7.37 (m, 14H, thread ArH plus
macrocycle pyridyl H), 7.65 (d, J = 7.8 Hz, 2H, thread pyridyl H), 7.96
(t, J = 7.8 Hz, 1H, macrocycle pyridyl H), 8.11 (t, J = 7.8 Hz, 1H,
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thread pyridyl H), 8.57 ppm (s, 2H, thread HC N); 13C NMR
=
(100 MHz, CDCl3, 298 K): d = 25.6, 28.4, 28.5, 29.4, 31.5, 34.5, 52.2,
55.3, 63.9, 67.4, 114.1, 120.8, 123.0, 124.1, 124.3, 124.6, 127.0, 128.5,
130.6, 141.5, 141.9, 143.3, 143.4, 145.9, 148.9, 149.0, 155.0, 158.2,
158.7 ppm; IR (KBr pressed pellet): n˜ = 3465, 2960, 2865, 1611, 1582,
1513, 1464, 1395, 1363, 1251, 1180, 1109, 1089, 1017, 840, 823, 637, 625,
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4054.
582 cmꢀ1
;
LRESI-MS:
m/z = 830
[Zn(L1L2)]2+
,
1759
[Zn(L1L2)](ClO4)+; HRFAB-MS (3-NOBA matrix): m/z =
12
1657.97065
(calcd
for
C
111
13CH132N6O264Zn
[(L1L2)Zn],
1657.97363).
Received: October 29, 2003 [Z53186]
Published Online: January 27, 2004
Keywords: coordination modes · rotaxanes · self-assembly ·
.
template synthesis · thermodynamic control
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[9] Reactions were monitored by electrospray mass spectrometry in
all cases and by 1H NMR spectroscopy for systems not contain-
ing paramagnetic metals.
[10] The L1 and L2 resonances in [Zn(L1L2)](ClO4)2] were distin-
guished by a combination of COSY and ROESY experiments.
[11] [Cd(L1L2)](ClO4)2·2 MeCN·1.5 Et2O:
Mr = 2098.82, yellow block, crystal size 0.15 0.12 0.10 mm,
monoclinic Cc, a = 31.636(2), b = 22.4269(14), c =
C124H153CdCl2N8O11.5,
22.2668(15) , b = 133.7570(10)8, V= 11410.8(13) 3, Z = 4,
1calcd = 1.222 Mgmꢀ3; MoKa radiation (graphite monochromator,
l = 0.71073 ), m = 0.300 mmꢀ1, T= 150(2) K. 36017 data (22989
unique, Rint = 0.03170, 1.27 < q < 28.968), were collected on a
Bruker SMARTApex CCD diffractometer by using narrow
frames (0.38 in w), and were corrected semiempirically for
absorption and incident beam decay. The structure was solved by
direct methods and refined by full-matrix least-squares on F2
values of all data (G. M. Sheldrick, SHELXTL manual, Siemens
Analytical X-ray Instruments, Madison WI, USA, 1994, version
5) to give wR = {ꢀ[w(F2oꢀFc2)2]/ꢀ[w(F2o)2]}1/2 = 0.1536, conven-
tional R = 0.0627 for F values of 22989 reflections with F2o >
2sF2o), S = 1.048 for 1371 parameters. Residual electron density
extremes were 1.12 and ꢀ0.89 eꢀ3. Hydrogens were added in
calculated positions and constrained to a Riding model. CCDC-
224059 contains the supplementary crystallographic data for this
paper. These data can be obtained free of charge via
bridge Crystallographic Data Centre, 12 Union Road, Cam-
bridge CB21EZ, UK; fax: (+ 44)1223-336-033; or deposit@
ccdc.cam.ac.uk).
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[12] Under identical experimental conditions the reduced thread,
H4L2, does not afford [Zn(L1H4L2)](ClO4)2, thus precluding the
possibility of a “slippage” mechanism.
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ꢀ 2004 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
1221