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A total of 1147 patients received ≥1 dose of drug and were included in the safety population for the 2 phase III trials; 564 patients received fidaxomicin.
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To avoid the possibility of data being collected for the 2 Phases at the same time, Phase 1 data collection was completed before the introduction of the EHR.
There are five different crystal structures for the R2O3 phase.
The annealing temperatures for the MoS2 phase transformation in this study are 250, 300, and 350 °C.
Further, no peak was observed for the Al2O3 phase in any of the XRD patterns.
We obtained average H (and E) values (in GPa) of 12.94 (464.95) for the WSi2 phase, 19.49 (214.52) for the matrix, 14.95 (142.84) for the Si rich phase, and 13.98 (138.56) for the Ge rich phase respectively; while average kc values (in MPa m0.5) were 1.37 for theWSi2, 0.52 for the matrix, 0.36 for the Si rich and 0.24 for the Ge rich phases respectively.
The growth directions in the lamellar eutectic are found to be 〈1 0 0〉 for the Cr3Si phase and 〈1 1 1〉 for the Cr solid-solution phase.
An obvious arrest by approximately 5.38% for the G0/G1 phase was observed compared with the GA-treated system.
On the basis of our experimental results, detailed formation mechanisms for the In2O3/InOOH phase and nanostructures were proposed.
As is known, the Raman spectra for the MnO2 phase and the Mn3O4 phase are located at 638.5 cm-1 and 652.5 cm-1, respectively [31].
Ab initio calculations for the B2 phase show a similar trend as calorimetric measurements but the magnitude is much smaller.
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