Presentation of Glycosyl Amino Acids
FULL PAPER
were run using an exponential decay constant of 8 ns and a simulation
length of 80 ns.
understanding the complex molecular processes between
glycopeptides and their biological targets.
X-Ray diffraction analysis[29]: Crystal data for 9: C47H50N2O12; Mw =
834.89; colorless prism of 0.25ꢆ0.25ꢆ0.22 mm; T=173 K; monoclinic;
space group P21/c; Z=2; a=13.5848(4) ꢃ, b=11.7140(3) ꢃ, c=
14.9527(4) ꢃ, b=112.8678(10)8; V=2192.44(10) ꢃ3; dcalc =1.265 gcmÀ3
;
Experimental Section
FACTHNUTRGNEUNG
(000)=884; l=0.71073 ꢃ (MoKa); m=0.091 mmÀ1; Nonius kappa CCD
diffractometer, q range 3.43–28.158, 18857 collected reflections, 9792
unique, full-matrix least-squares (SHELXL97),[30] R1 =0.0535, wR2 =
0.1128, (R1 =0.0874, wR2 =0.1302 all data), goodness of fit=1.014, resid-
ual electron density between 0.23 and À0.245eꢃÀ3. Hydrogen atoms
fitted at theoretical positions.
General Procedures: Solvents were purified according to standard proce-
dures. Analytical TLC was performed using Polychrom SI F254 plates.
Column chromatography was performed using Silica gel 60 (230–400
mesh). 1H and 13C NMR spectra were recorded with Bruker ARX 300
and Bruker AVANCE 400 spectrometers. 1H and 13C NMR spectra were
recorded in CDCl3 with TMS as internal standard or in D2O (chemical
shifts referenced to the internal solvent signals and reported in ppm on
the d scale; coupling constants in Hz). Assignment of all separate signals
Crystal data for compound 15·Et2O: C49H68N4O11; Mw =889.08; colorless
prism of 0.27ꢆ0.15ꢆ0.12 mm; T=173 K; monoclinic; space group P21;
Z=2; a=12.2297(6) ꢃ, b=15.0023(8) ꢃ, c=13.3856(5) ꢃ, b=98.902(3)8;
V=2426.3(2) ꢃ3; dcalc =1.217 gcmÀ3; F
ACHTNUTRGNE(UNG 000)=956; l=0.71073 ꢃ (MoKa);
1
for the final compounds in the H NMR spectra was made on the basis of
m=0.086 mmÀ1; Nonius kappa CCD diffractometer, q range 2.05–28.088,
21769 collected reflections, 5820 unique, full-matrix least-squares
(SHELXL97),[30] R1 =0.0618, wR2 =0.0990, (R1 =0.1254, wR2 =0.1166 all
data), goodness of fit=1.047, residual electron density between 0.293 and
À0.179eꢃÀ3. Hydrogen atoms fitted at theoretical positions.
coupling constants, ge-COSY and ge-HSQC experiments with a Bruker
AVANCE 400 spectrometer. The NMR data were processed with Mestre
Nova software (Mestrelab Research, Spain). Melting points were deter-
mined with a Bꢅchi SMP-20 melting point apparatus. Microanalyses were
carried out with a CE Instruments EA-1110 analyzer and are in good
agreement with the calculated values. Optical rotations were measured
with a Perkin–Elmer 341 polarimeter. Electrospray mass spectra were re-
corded with a microTOF-Q-BRUKER connected to a Waters 996 photo-
diode array detector with H2O or MeOH as carrier solvents. The synthet-
ic procedures for all new compounds as well as their physical properties
are detailed in the Supporting Information.
Acknowledgements
We thank the Ministerio de Ciencia e Innovaciꢁn and FEDER (project
CTQ2009–13814/BQU and FPI grant of V. J. S.), the Universidad de La
Rioja (project EGI10/65), and the Gobierno de La Rioja (Colabora 2010/
05). F. R. thanks the CSIC for his JAE-Doc Program contract. We also
thank CESGA for computer support.
NMR experiments: NMR experiments were recorded with a Bruker
Avance 400 spectrometer at 298 K. Magnitude-mode ge-2D COSY spec-
tra were recorded with gradients and using the cosygpqf pulse program
with 90 degree pulse width. Phase-sensitive ge-2D HSQC spectra were
recorded using z-filter and selection before t1, removing the decoupling
during acquisition by use of invigpndph pulse program with CNST2
(JHC)=145. 2D NOESY experiments were made using phase-sensitive
ge-2D NOESY with WATERGATE for H2O/D2O (9:1) spectra. Selective
ge-1D NOESY experiments were carried out using the 1D-DPFGE NOE
pulse sequence. NOE intensities were normalized with respect to the di-
agonal peak at zero mixing time. Experimental NOEs were fitted to
[2] a) L. Shao, Y. Luo, D. J. Moloney, R. S. Haltiwanger, Glycobiology
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[4] F. Corzana, A. Fernꢈndez-Tejada, J. H. Busto, G. Joshi, A. P. Davis,
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[5] a) A. Fernꢈndez-Tejada, F. Corzana, J. H. Busto, G. Jimꢇnez-Osꢇs, J.
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a double exponential function, f(t)=p0 (eÀp1t
)ACTHNGUTERNNUG
being adjustable parameters.[13] The initial slope was determined from the
first derivative at time t=0, f’(0)=p0p2. From the initial slopes, interpro-
ton distances were obtained by employing the isolated spin pair approxi-
mation.
MD simulations in explicit water: Simulations were performed by using
the AMBER 9 program package (parm99),[22] which was implemented
with GLYCAM 06 parameters.[23] Unrestrained MD simulations were car-
ried out in the presence of explicit TIP3P water molecules.[24] RESP
atomic charges[25] for the glycopeptides were derived by applying the
RESP module of AMBER to the HF/6–31G(d) ESP charges calculated
with Gaussian 08.[26] The simulations were run with the PMEMD module
of AMBER with SHAKE algorithm,[27] using periodic boundary condi-
tions, a 2 fs time step, a temperature of 300 K, a Langevin type thermo-
stat for temperature control, and constant pressure of 1 atm. A 9 ꢃ cut-
off was applied to the Lennard-Jones interactions, and Ewald sums for
the treatment of the electrostatic interactions.[28] An initial 2500 cycles of
minimization (combining steepest descent with conjugate gradient) were
run on both systems by first restraining the atoms of the complex. The
whole system was then minimized using 2000 cycles. This first step was
followed by 200 ps of dynamics at constant volume with weak positional
restrains on the complex (10 kcalmolÀ1·ꢃ2). In this step, the system was
heated from 100 to 300 K. The restrains on the solute were removed and
200 ps MD simulations were run at 300 K and 1 atm to obtain the appro-
priate density. Finally, 20 ns MD simulations were run using the condi-
tions mentioned above.
MD simulations: NOE-derived distances were included as time-averaged
distance restraints, and scalar coupling constants (J) as time-averaged
À1/6
coupling restraints. A <rÀ6
>
average was used for the distances and
a linear average was used for the coupling constants. Final trajectories
Chem. Eur. J. 2012, 18, 5096 – 5104
ꢂ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
5103