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Figure 4
X-ray intensity versus wavevector transfer for the SmC*FI2 phase of MHDDOPTCOB. The splitting becomes resolvable for the second-order peak. Reprinted figure with permission from Mach et al. (1999 ![]() |
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Figure 4
X-ray intensity versus wavevector transfer for the SmC*FI2 phase of MHDDOPTCOB. The splitting becomes resolvable for the second-order peak. Reprinted figure with permission from Mach et al. (1999 ![]() |