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In the systems with cubic symmetry, the ratios of reciprocal d of observed peaks are √n1:√2:√3, and the numbers (n1, n2, and n 3) inside √, or those times integer, should correspond to h2, k2, l2 when the diffraction is assigned to (hkl) planes. Because the (hkl) planes with h2, k2, l2, 7 and 15 are not possible with any cubic systems, the sequence of numbers must be doubled. Indexation of diffractions assigned to (321) and (521) was made in this way see Figures 2 and 4, and the Supporting Information, Figures S1, S2, and S4-S6
-
2 = 7 and 15 are not possible with any cubic systems, the sequence of numbers must be doubled. Indexation of diffractions assigned to (321) and (521) was made in this way (see Figures 2 and 4, and the Supporting Information, Figures S1, S2, and S4-S6).
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-
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89
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0036501376
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but this case is a transition between two micellar type Cub phases
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Percec, V.; Holerca, M. N.; Uchida, S.; Cho, W.-D.; Ungar, G.; Lee, Y.; Yeardley, D. J. P. Chem.-Eur. J. 2002, 8, 1106-1117, but this case is a transition between two micellar type Cub phases.
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Percec, V.1
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Yeardley, D.J.P.7
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90
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47049119819
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For all BABH-n, a broad halo was detected in the small-angle region at temperatures even in the isotropic liquid I phase in the vicinity of the Cub/SmC phase, and the spacing is plotted with symbols V or T. The selected patterns are displayed in the Supporting Information, Figure S7. The presence of such a halo indicates that there still remain the constituent aggregates that construct the Cub/SmC phase structure, which would gradually collapse in the higher-temperature region. A similar observation was reported for other Cub-phase-forming materials (see refs 15e,f, 25, 27c,d, and 56b, which also exhibit the so-called DSC hump both on heating and on cooling; in BABH-n, however, the transition peak into the I phase was followed by not a clear hump but only a tail extended at the higher temperature side see Figure 1
-
For all BABH-n, a broad halo was detected in the small-angle region at temperatures even in the isotropic liquid I phase in the vicinity of the Cub/SmC phase, and the spacing is plotted with symbols V or T. The selected patterns are displayed in the Supporting Information, Figure S7. The presence of such a halo indicates that there still remain the constituent aggregates that construct the Cub/SmC phase structure, which would gradually collapse in the higher-temperature region. A similar observation was reported for other Cub-phase-forming materials (see refs 15e,f, 25, 27c,d, and 56b), which also exhibit the so-called DSC "hump" both on heating and on cooling; in BABH-n, however, the transition peak into the I phase was followed by not a clear hump but only a tail extended at the higher temperature side (see Figure 1).
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93
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0019327168
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(b) Umemura, J.; Cameron, D. G.; Mantsch, H. H. Biochim. Biophys. Acta 1980, 602, 32-44.
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Lee, W.K.1
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(b) Wang, F. C.; Feve, M.; Lam, T. M.; Pascault, J.-P. J. Polym. Sci., Part B: Polym. Phys. 1994, 32, 1305-1313.
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Wang, F.C.1
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-
97
-
-
47049117062
-
-
Absorption in the range 3030-3150 cm-1, which has two evident peaks at 3040 and 3070 cm-1, is assigned to the C-H stretching vibrations of the benzene ring, and a shoulder peak around 3200 cm-1 is probably the two-phonon band of the C=O fundamental vibration observed at around 1640 cm-1 48b Thus, the curve-fitting procedure was performed in the range 3250-3600 cm-1
-
-1.
-
-
-
-
98
-
-
47049096539
-
-
free N-H being the coefficients for hydrogen-bonded and free N-H vibration bands, respectively) depended on n and ranged between 5.1 and 9.7 (see the Supporting Information, Table S2). More detailed procedures are described in the Supporting Information, Figure S13.
-
free N-H being the coefficients for hydrogen-bonded and free N-H vibration bands, respectively) depended on n and ranged between 5.1 and 9.7 (see the Supporting Information, Table S2). More detailed procedures are described in the Supporting Information, Figure S13.
-
-
-
-
99
-
-
0000661384
-
-
Demus, D, Goodby, J, Gray, G. W, Spiess, H.-W, Vill, V, Eds, Wiley-VCH: Weinheim, Germany
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Fairhurst, C. E.; Fuller, S.; Gray, J.; Holms, M. C.; Tiddy, G. J. T. In Handbook of Liquid Crystal; Demus, D., Goodby, J., Gray, G. W., Spiess, H.-W., Vill, V., Eds.; Wiley-VCH: Weinheim, Germany, 1998; Vol. 3, pp 341-392.
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Fairhurst, C.E.1
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Holms, M.C.4
Tiddy, G.J.T.5
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102
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47049115799
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-
CH2) were evaluated for 70 °C, but we used without correcting the temperature effect, because of the expectation that the partial are more or less reduced for the alkyl chains with one end attached to an aromatic core such as in our case.
-
CH2) were evaluated for 70 °C, but we used without correcting the temperature effect, because of the expectation that the partial volumes are more or less reduced for the alkyl chains with one end attached to an aromatic core such as in our case.
-
-
-
-
103
-
-
5244367703
-
-
8th ed, Stecher, P. G, Windholz, M, Leahy, D. S, Eds, Merck: Rahway, NJ
-
Merck Index, 8th ed.; Stecher, P. G., Windholz, M., Leahy, D. S., Eds.; Merck: Rahway, NJ, 1968.
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(1968)
Merck Index
-
-
-
104
-
-
47049093445
-
-
38b,c
-
38b,c
-
-
-
-
105
-
-
0000008971
-
-
(a) Donnio, B.; Heinrich, B.; Gulik-Krzywicki, T.; Delacroix, H.; Guillon, D.; Bruce, D. W. Chem. Mater. 1997, 9, 2951-2965.
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Donnio, B.1
Heinrich, B.2
Gulik-Krzywicki, T.3
Delacroix, H.4
Guillon, D.5
Bruce, D.W.6
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106
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-
30944457103
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-
(b) Kutsumizu, S.; Saito, K.; Nojima, S.; Sorai, M.; Galyametdinov, Y. G.; Galyametdinova, I.; Eidenschink, R.; Haase, W. Liq. Cryst. 2006, 33, 75-84.
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Galyametdinova, I.6
Eidenschink, R.7
Haase, W.8
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107
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47049106053
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-
Strictly speaking, the two alkyl chains might be obliquely directed with respect to the long axis of the core part, especially in the SmC phase, and thus the molecules would have somewhat of a zig-zag shape. In this discussion, however, we ignore this fact and regard the molecular shape as being rodlike, if the alkyl and hydrogen-bonding effects are equally balanced. Also, in Figure 12, only a half of the molecule is schematically depicted for clarity.
-
Strictly speaking, the two alkyl chains might be obliquely directed with respect to the long axis of the core part, especially in the SmC phase, and thus the molecules would have somewhat of a zig-zag shape. In this discussion, however, we ignore this fact and regard the molecular shape as being rodlike, if the alkyl and hydrogen-bonding effects are equally balanced. Also, in Figure 12, only a half of the molecule is schematically depicted for clarity.
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-
-
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