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Solid State NMR Studies of Complex Two Dimensional Structures: Polyelectrolyte Multilayers and Layered Silicates Robert Graf, Mark McCormick, Linda Reven*, Niklas Hedin+, Bradley F. Chmelka+ and Hans Wolfgang Spiess Max-Planck-Institut für Polymerforschung, Postfach 3148, 55021 Mainz, Germany * Dep. of Chemistry, McGill University, 801 Sherbrooke Street West, Montreal, Quebec, Canada H3A 2K6 + Dep. of Chemical Engineering, University of California, Santa Barbara, CA 93106, USA Introduction Structure of Surfactant Controlled Silicate Layers The 29Si CPMAS spectrum of the layered silicate sample exhibits five different sites (left). The chemical bonded network was investigated using INADEQUATE measurements [3]. Exploring the CSA of these sites provides a direct method to distinguish the Q3 and Q4 sites present in the sample. The inherently low sensitivity of NMR hampers in many cases studies of low dimensional entities such as films or molecular layers. However, fast MAS in combination with advanced recoupling techniques are able to increase the signal to noise ration sufficiently such that structure and dynamics of polyelectrolyte multilayers (PEM) [1] or surfactant controlled silicate layers can investigated. Due to the complex structure of the samples, the most robust recoupling sequences available had to be chosen to obtain artefact free results. The double-quantum NMR experiments have been recorded using the Back-to-Back sequence [2] in the fast MAS limit, whereas the SUPERNMR scheme [4] has been applied for chemical shift anisotropy recoupling. -95 Polyelectrolyte Multilayer Anionic Substrate Polycation Solution Q3 PSS 500 MHz Polycation Solution After Drying 4 H 3C 8 10 O 12 14 H H N + CH 3 OS Double Quantum Dimension [ppm] Double Quantum Dimension [ppm] T1 [msec] 2 H H O H H H H 16 9 8 7 6 5 4 3 2 6 x -x 8 Spin-Lattice Relaxation 14 1 2 3 16 4 5 6 8 7 6 5 4 3 2 1 7 8 9 10 C 110 550 100 O 350 300 250 3 4 5 6 7 Number of Layers 8 9 10 C S H H O H H H H H 3C H H N + -210 CH3 La yer 2 90 L aye r 3 80 La yer 4 70 L aye r 5 60 L aye r 6 50 L aye r 7 40 L aye r 8 1 2 3 4 5 6 7 8 9 10 C L aye r 9 Number of Layers Water adsorbed in PEMs, shows oscillatory relaxation times and chemical shifts depending on the material of the last layer. Its T1 relaxation is in the fast motion limit . Lay er 10 8 7 1H 6 5 4 3 12 10 8 6 4 2 0 pp m -200 5 .0 Wate r Chemi cal Shi ft [ppm ] Linewidth at FWHH [Hz] 400 -220 O L aye r 1 4 .8 4 .6 4 .4 b u lk PDADM AC 4 .2 3 .8 b u lk PS S 3 .6 1 2 ppm MAS NMR Spectra 1H 3 4 5 6 7 8 L a y e r Nu m b e r 9 10 -95 -100 -105 -110 II. Q3 σiso= -100 ppm δ = 44 ppm η = 0.23 σiso= -96 ppm δ = 60 ppm η = 0.23 0 -50 -100 -150 ppm single quantum dimension Chemical Shift Complexation: (i) Polycation-polyanion complexation of polyelectrolyte multi-layers (PEM) is similar to that in the bulk polyelectrolyte complex (PEC). (ii) Water-polymer association in PEMs is much stronger than in PEC. Polymer Dynamics: (i) Addition of water increases the polymer mobility in PEMs but not in the PEC. (ii) Enhanced polymer mobility is observed for hydrated PDADMAC-capped films relative to PSS capped films. (iii) This oscillation in the polymer mobility dampens and is superimposed on a gradient of decreasing mobility with film thickness. No changes with layer number are observed for dry films. III. Adsorbed Water: (i) Mobility of adsorbed water is more restricted in PEMs than in the PEC. (ii) Water mobility is lower and water content is higher in PSS capped films as compared to PDADMAC capped PEMs. (iii) 1H NMR peak intensity increases monotonically and its chemical shift oscillates between the PEC bulk and the bulk PDADMAC value. direct neighbor Next nearest neighbor -115 ppm Combining short range spatial information from NMR methods 29Si I. δ = 10 ppm -190 b u lk PE C 4 .0 Si site ppm -230 T1 relaxation measurements of PDADMAC-PSS multilayers find the polymers to move in the slow motion regime and exhibit an oscillatory behavior the relaxation times approaching the value of the polyelectrolyte complex. Linewidth (apparent 1/T2) 600 σiso=-102.5 ppm pulse scheme of CSA recoupling experiment Number of Layers Single Quantum Dimension [ppm] Spin-Lattice Relaxation T1 [msec] t1=n·τR σiso= -113.5 ppm 200 12 1H double quantum NMR indicates that the layered structure of PDADMAC-PSS multi-layers is strongly interdigitating and resembles the polyelectrolyte complex. 2 -x x τR 10 Single Quantum Dimension [ppm] 1 DD CP 600 400 9 1 Overlapping peaks and weak signal intensities hamper the acquisition of static powder spectra. CSA recoupling pulse program [4] (shown at the left hand side) provides access to the static line shapes of the individual sites, and thus to the complete set of CSA parameters . sites 18 18 200 and Q4 Dipolar Decoupling Polyanion Solution 6 Q3 PSS 700 MHz 800 Polyelectrolyte Complex Formation 4 ppm PDADMAC 700MHz Aqueous Rinse 2 -115 Q4 sketch of CSA tensors in PDADMAC 500MHz 1000 Polyanion Solution -110 σiso= -108 ppm double quantum dimension After 3 cycles -105 CP MAS spectrum of surfactant controlled layered silicate NMR Investigations of Polyelectrolyte Multi-Layers Polyelectrolyte Complex -100 Q4 double quantum spectra, recorded with various DQ recoupling times, provide the nearest and next nearest neighbor relation (given in the table) between the sites of the sample, leading to a proposed structure shown right. MD simulation and quantum chemical (QC) computations have been used to verify the structure. with MD simulations and QC computations can unravel low dimensional structures yet inaccessible to common scattering methods. References [1] M. McCormick, R.N. Smith, R. Graf, C.J. Barrett, L. Reven and H.W. Spiess, Macromolecules 36, (2003) 3616. [2] M. Feike, D.E. Demco, R. Graf, J. Gottwald, S. Hafner, and H.W. Spiess, J. Magn. Reson. A 122, (1996) 214. [3] S.C. Christiansen, D. Zhao, M.T. Janicke, C.C. Landry, G.D. Stucky, and B.F. Chmelka, J. Am. Chem. Soc. 123, (2001) 4519. [4] S-F. Liu, J-D. Mao, and K. Schmidt-Rohr, J. Magn. Reson. 155,(2002) 15.