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1642452291
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note
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Dependent on the functionality, at high CMS:S ratios some processing parameters such as solubility and the ability to achieve complete postpolymerization functionalization become problematic.
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31
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0033612004
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38
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1642493314
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note
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19 We find that within this range the variation of our quantitative results is marginal (e.g., volume fractions vary by about 1%).
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39
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1642452289
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note
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In general, we refrained from casting the samples from solution to avoid kinetic entrapment effects caused by selectivity of the solvent to either block. Nevertheless, we note that annealed samples cast from toluene still exhibited the same SAXS characteristics as those annealed from the powder form, which therefore leads us to believe that the investigated melts were in equilibrium.
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40
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0003552279
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Mark, J. E. Ed.; American Institute of Physics: Woodbury, NY
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Physical Properties of Polymers Handbook; Mark, J. E. Ed.; American Institute of Physics: Woodbury, NY, 1996.
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41
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1642493315
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note
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In these calculations we neglected the difference between CMS and styrene. Calculated volume fractions of the Anth functionality in PS/S-Anth/CMS (19, 7%, 13%) and (19, 12%, 8%) are 0.16 and 0.26, respectively. For data pertaining to the fully converted PS/S-Anth (19, 20%) and (25, 50%) see Table 2.
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47
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1642493317
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note
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2I vs q (instead of I vs q) under the assumption that the polymers feature lamellar morphology, based on the range of calculated volume fractions of the functionalized blocks (0.36-0.55) and mean-field theory.
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48
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1642493316
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note
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This situation does not result from lack of electron density contrast that may arise from a small number of Anth functionalities in the PS/S-Anth (27: 13, 17%) polymer; other polymers that feature the same low functionality content but longer functionalized blocks (with up to twice the total number of Anth units per polymer) do not exhibit a distinct SAXS peak as well.
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49
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1642574744
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note
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func-PS = 0.40), as in perfectly symmetric diblock copolymers it is completely absent.
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52
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1642452290
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note
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For consistency, all the variables appearing in eqs 2 and 3 were also evaluated using the topological indices.
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54
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0034620457
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For a detailed discussion and references, see: Ren, Y.; Lodge, T. P.; Hillmyer, M. A. Macromolecules 2000, 33, 866
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Ren, Y.1
Lodge, T.P.2
Hillmyer, M.A.3
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0037035689
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Ren, Y.; Lodge, T. P.; Hillmyer, M. A. Macromolecules 2002, 35, 3889.
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Ren, Y.1
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56
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1642574743
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note
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All precursors to polymers of series B were synthesized from the same batch of PS block, with exactly the same styrene/CMS mixture composition (i.e., comonomer quantities); thus, the differences between the functionalized blocks of these polymers resulted only from different polymerization times.
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57
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1642493318
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note
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Despite the lack of secondary scattering peaks in the SAXS curves of the polymers of series B, we consider the melts of these polymers, quenched from 150 °C, as phase-separated, since only weak dependence of the scattering behavior on annealing temperature or annealing scheme was observed. For example, annealing at 150 °C for a few hours, then at 125 °C for 2 days, and then slowly cooling the samples to room temperature did not result in a significant change in the principal peak location/width or appearance of secondary scattering peaks. Therefore, the absence of secondary secondary scattering peaks is attributed to weak segregation (and possibly also to low electron density contrast) rather than to disorder.
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