Masuda and Stephan
325
Scheme 1. Bridged Rh–N2 complexes.
Scheme 2. Terminal Rh–N2 complexes.
collected (4.5° < 2θ < 45–50.0°). The intensities of reflec-
tions within these frames showed no statistically significant
change over the duration of the data collections. The data
were processed using the SAINT and XPREP processing
packages. An empirical absorption correction based on re-
dundant data was applied to each data set. Subsequent solu-
tion and refinement was performed using the SHELXTL
solution package.
in pentane (5 mL) and again filtered through Celite®. Cooling
the pentane solution to –35 °C gave 263 mg of a dark brown
crystalline solid after work-up. Yield: 38%. IR (KBr
pellet, cm–1): 2175 (νNN), 1535 (νNC). 1H NMR (0 °C): 6.98–
7.13 (m, 6H, m, p-Ar, C7D7H), 5.12 (s, 1H, CH), 3.73 (br
Structure solution and refinement
Non-hydrogen atomic scattering factors were taken from
the literature tabulations (17, 18). The heavy atom positions
were determined using direct-methods employing the
SHELXTL direct-methods routine. The remaining non-
hydrogen atoms were located from successive difference
Fourier map calculations. The refinements were carried out
by using full-matrix least-squares techniques on F, minimiz-
ing the function ω (Fo – Fc)2 where the weight ω is defined
sept, 2H, CH, JH-H = 7 Hz), 3.46 (br sept, 2H, CH, JH-H
7 Hz), 3.27 (br d, 2H, HC=CH, JH-H = 10 Hz), 1.59 (6H,
Me), 1.58 (d, 6H, i-Pr, JH-H = 7 Hz), 1.47 (d, 6H, i-Pr, JH-H
=
=
7 Hz), 1.41 (br m, 4H, CH2), 1.20 (d, 6H, i-Pr, JH-H = 7 Hz),
1.14–1.29 (m, 8H, CH2), 1.02 (d, 6H, i-Pr, JH-H = 7 Hz). 13C
NMR (25 °C, partial): 157.8, 152.0, 143.1, 142.7, 141.6,
130.3, 127.8–129.0 (m, obscured by toluene-d8) 126.2,
125.4, 123.9, 123.7, 123.3, 97.3 (C-H, 74.9, (broad s, H-
C=C-H), 30.7, 29.5, 28.9, 28.1, 26.5, 25.8, 25.0, 24.7, 24.4,
23.6. Anal. calcd. for C37H55N4Rh: C 67.46, H 8.42, N 8.50;
found: C 67.46, H 8.49, N 8.30.
2
2
as 4Fo /2σ(Fo ), and Fo and Fc are the observed and calcu-
lated structure factor amplitudes. In the final cycles of each
refinement, all non-hydrogen atoms were assigned aniso-
tropic temperature factors in the absence of disorder or
insufficient data. In the latter cases, atoms were treated
isotropically. C-H atom positions were calculated and al-
lowed to ride on the carbon to which they are bonded assum-
ing a C—H bond length of 0.95 Å. H atom temperature
factors were fixed at 1.10 times the isotropic temperature
factor of the C atom to which they are bonded. The H-atom
contributions were calculated, but not refined. The locations
of the largest peaks in the final difference Fourier map cal-
culation as well as the magnitude of the residual electron
densities in each case were of no chemical significance. Ad-
ditional details are provided in the supplementary data.3
X-ray data collection and reduction
Crystals were manipulated and mounted in capillaries in a
glovebox, thus maintaining a dry, O2-free environment for
each crystal. Diffraction experiments were performed on a
Siemens SMART System CCD diffractometer. The data
were collected in a hemisphere of data in 1448 frames with
10 s exposure times. The observed extinctions were consis-
tent with the space groups in each case. The data sets were
3 Supplementary data may be purchased from the Directory of Unpublished Data, Document Delivery, CISTI, National Research Council
CCDC 252431 contains the crystallographic data for this manuscript. These data can be obtained, free of charge, via
ww.ccdc.cam.ac.uk/conts/retrieving.html (or from the Cambridge Crystallographic Data Centre, 12 Union Road, Cambridge CB2 1EZ, UK;
fax +44 1223 336033; or deposit@ccdc.cam.ac.uk).
© 2005 NRC Canada