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range=580–380,000 gmolÀ1); Mn,SEC values of the PMLABzs,
PMLAAlls, and PMLAMes were uncorrected for the possible difference
in hydrodynamic radius versus polystyrene.
The molar mass values of PMLABzs, PMLAAlls, and PMLAMes samples
were also determined by 1H NMR spectroscopic analysis in CDCl3
from the relative intensities of the signals of the PMLABz main-
chain methine hydrogen signals (-OCH(CO2Bz)CH2, d=5.58 ppm),
PMLAAll main-chain methine (-OCH(CO2All)CH2, d=5.52 ppm),
PMLAMe main-chain methine (-OCH(CO2Me)CH2, d=5.50 ppm), and
those of the isopropyl chain-end (-OCH(CH3)2, d=1.24 ppm).
iPrO-PMLAAll-H: H NMR (500 MHz; CDCl3, 258C): d=5.88 (m, 1nH;
CH2CH=CH2), 5.52 (m, 1nH; CH2CH(CO2All)O), 5.31 and 5.25 (d and
d, J=17 and 10 Hz, respectively (geminal proton-proton couplings
were not observed), 2nH; CH2CH=CH2), 4.64 (d, J=5 Hz, 2nH;
CH2CH=CH2), 3.41 (m, 1H; (CH3)CHO), 3.00 (m, 2nH;
CH2CH(CO2All)O), 1.24 ppm (m, 6H; (CH3)CHO) (Figure 6); 13C{1H}
NMR (125 MHz; CDCl3, 258C): d=168.1 and 167.8 (C=O), 131.3
(CH2CH=CH2), 119.0 (CH2CH=CH2), 68.7 (CH2CH(CO2All)O), 66.4
(CH2CH=CH2), 41.8 ((CH3)CHO), 35.4 (CH2CH(CO2All)O), 21.7 ppm
((CH3)CHO) (Figure S6).
1
iPrO-PMLAMe-H: H NMR (500 MHz; CDCl3, 258C): d=5.50 (m, 1nH;
1
Monomer conversions were calculated from H NMR spectra of the
CH2CH(CO2CH3)O), 3.76 (m, 3nH; CH2CH(CO2CH3)O), 3.45 (m, 1H;
(CH3)CHO), 3.01 (m, 2nH; CH2CH(CO2 CH3)O), 1.26 ppm (m, 6H;
(CH3)CHO) (Figure 2); 13C{1H} NMR (125 MHz; CDCl3, 258C): d=
168.7 and 168.3 (C=O), 68.7 (CH2CH(CO2CH3)O), 53.0
(CH2CH(CO2CH3)O), 35.6 (CH2CH(CO2CH3)O), 34.3 ((CH3)CHO),
22.5 ppm ((CH3)CHO) (Figure 3).
crude polymer samples in CDCl3 by using the integration (Int.) ratio
Int.PMLAR/[Int.PMLAR+Int.MLAR] of the methine hydrogen signals
(-OCH(CO2R)CH2: d=5.50–5.58 ppm for polymers and d=4.88 ppm
for monomers).
MALDI-ToF mass spectra were recorded at the CESAMO (Bordeaux,
France) with a Voyager mass spectrometer (Applied Biosystems)
equipped with a pulsed N2 laser source (337 nm) and a time-de-
layed extracted ion source. Spectra were recorded in the positive-
ion mode using the reflectron mode and with an accelerating volt-
age of 20 kV. A THF solution (1 mL) of the matrix (trans-3-indole-
acrylic acid, IAA; Aldrich, 99%) and a MeOH solution of the cation-
ization agent (NaI, 10 mgmLÀ1) were prepared. A fresh solution of
the polymer samples in THF (10 mgmLÀ1) was then prepared. The
three solutions were then rapidly combined in a 1:1:10 v/v
[matrix]/[sample]/[cationization agent] ratio. An aliquot (1–2 mL) of
the resulting solution was deposited onto the sample target and
vacuum-dried.
Computational details
All calculations were performed with the TURBOMOLE program
package using density functional theory (DFT).[28–31] The gradient
corrected density functional BP86 in combination with the resolu-
tion identity approximation (RI)[32,33] was applied for the geometry
optimizations of stationary point. A triple-z zeta valence quality
basis set def-TZVP was used for all atoms.[34] The stationary points
were characterized as energy minima (no negative Hessian eigen-
values) by vibrational frequency calculations at the same level of
theory. The results of calculations (total electronic energies of eight
intermediates and zero-point energy corrections) are presented in
Figure 14 and Table S7.
Differential scanning calorimetry (DSC) analyses were performed
with a Setaram DSC 131 apparatus calibrated with indium, at
a
rate of 108CminÀ1
,
under continuous flow of helium
(25 mLminÀ1), using aluminum capsules. The thermograms were
recorded according to the following cycles: À50 to 508C at
108CminÀ1; 50 to À508C at 108CminÀ1; À508C for 5 min; À50 to
Acknowledgements
200 or 2508C at 108CminÀ1; 200 to 308C at 108CminÀ1
.
The authors gratefully thank the CNRS and the Region Bre-
tagne for supporting part of this research (Ph.D. grant to
Statistical analysis and model fitting were performed by using soft-
ware OriginPro 8 from OriginLab Corporation and Mk1 and Mk2
models defined previously.[18]
1
C.G.J.). We thank Romain Ligny for performing VT H and DOSY
NMR spectroscopic analysis of complex 1d.
General procedure for the ROP of rac-MLAR
Keywords: density functional calculations
·
lactones
·
polymers · ring-opening polymerization · yttrium
In a typical experiment (Table 1, entry 3), a Schlenk flask was
charged in a glovebox with a solution of complex 1a (6.3 mg,
5.82 mmol) in toluene (0.58 mL), then iPrOH (0.50 mL, 5.82 mmol,
1.0 equiv vs. 1a) was added under stirring. After 5 min, rac-MLABz
was added rapidly (120 mg, 0.58 mmol, 100 equiv) and the mixture
was stirred at 208C for the appropriate time. The reaction was
quenched by addition of acetic acid (ca. 10 mL of a 1.6 mol·LÀ1 so-
lution in toluene). The resulting mixture was concentrated to dry-
ness under vacuum and the conversion was determined by
1H NMR spectroscopic analysis of the residue in CDCl3. The crude
polymer was then dissolved in CH2Cl2 (ca. 1 mL) and precipitated
in cold pentane (ca. 5 mL), filtered and dried under vacuum at
458C overnight (typical isolated yield 90–95%). The final polymer
was then analyzed by NMR, SEC, and DSC analyses (Table 1).
iPrO-PMLABz-H: 1H NMR (500 MHz; CDCl3, 258C): d=7.33 (br m,
5nH; C6H5), 5.55 (br m, 1nH; CH2CH(CO2Bz)O), 5.14 (br s, 2nH;
OCH2C6H5), 4.56 (br m, 1H; OCH(CH3)2), 2.94 (br m, 2nH;
CHCH2C(O)O), 1.24 ppm (m, 6H; OCH(CH3)2) (Figure 5); 13C{1H} NMR
(125 MHz; CDCl3, 258C): d=168.2–168.0 (C=O), 135.1 (C8), 128.3–
128.7 (C9–11), 68.8 (C(O)CH2CH(CO2Bz)O), 67.6 (OCH2C6H5), 65.7
((CH3)2CHO), 35.4 (OC(O)CH2CH), 20.9 ppm ((CH3)2CHO) (Figure S5).
[2] J. W. Kramer, D. S. Treitler, E. W. Dunn, P. M. Castro, T. Roisnel, C. M.
[3] C. G. Jaffredo, Y. Chapurina, S. M. Guillaume, J.-F. Carpentier, Angew.
[6] For leading reviews on stereoselective ROP of b-lactones, see: a) C. M.
[8] a) C.-X. Cai, A. Amgoune, C. W. Lehmann, J.-F. Carpentier, Chem.
Bouyahyi, A. Amgoune, C. M. Thomas, A. Bondon, I. Pillin, Y. Grohens, J.-
1872–1883; e) J. S. Klitzke, T. Roisnel, E. Kirillov, O. d. L. Casagrande, J.-F.
Chem. Eur. J. 2016, 22, 7629 – 7641
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