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0012080389
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note
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We showed in Ref. 17 that the growing structures were self-similar, regardless of time and quench depth. Thus, the prefactor must be the same for all of the quenches.
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52
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0012077001
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note
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Two independent runs were conducted on B2 at 35 °C. The fluctuation relaxation stage was clearly identified in only one of the runs.
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53
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0012049837
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note
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-1, respectively. We were able to begin the standard deviation procedure at higher q, because the detector was offset for these two experiments. This allowed measurements of the scattering intensity at higher q.
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54
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0012081222
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note
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-1 range.
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55
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0012018463
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note
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merge at both very early and late times was not possible. At early times, the small increases in the scattering intensity were of the same order as the noise in the data. At late times, the merge point moved to q-values near the high q limit of our SANS instrument.
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56
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0012019598
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note
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This includes earlier work on multicomponent polymer blends described in Refs. 16-18.
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57
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0012019599
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note
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i (3809 for B1 and B2, and 3704 for B3) in our comparisons of theory and experiment.
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58
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0012018196
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note
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The theoretical curves for the three blend are nearly indistinguishable in the range of interest (ordinate difference in < 0.03). For simplicity, a single curve (the average between the three theoretical curves) is shown.
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62
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0012049916
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note
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i [3809 for Fig. 10(a) and 3704 for Fig. 10(b)]. Thus the small changes in the monomer volumes with changing T and P are not accounted for in this figure.
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66
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0012081224
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note
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The 45 °C quench on the B2 sample lay just outside, but within experimental error of the pseudospinodal.
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67
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0012019418
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note
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s = 0.00782) and the average value of N (3809 for B1 and B2 and 3704 for B3).
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68
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0012080390
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note
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Identification of equipment and materials does not imply recommendation by the National Institute of Standards and Technology.
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