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The surface viscosities of both straight and mixed monolayers exhibit a maximum in the condensed untilted LS phase at pi = 20 mN/m.
As previously noted, pressure favors the smaller LS complexes, thus it stabilizes the LS phase of compound [35].
The LS phase was found to be stable at high pressure above the red line p ↓. Conversely HS phase is stable at lower pressures below the blue line p ↑.
Both these pathways are induced by progesterone withdrawal during the LS phase.
We propose that these pathways are activated in the endometrium after progesterone withdrawal in the LS phase, to up-regulate AM for endometrial repair.
To test this hypothesis, we subjected P endometrium to a previously described ex vivo model of progesterone antagonism (57), to mimic progesterone withdrawal in the LS phase.
Similar(49)
The L phase is shown to be a rational approximant of the icosahedral phase.
The thermodynamic phase diagrams for both systems (ECTFE/DEP and ECTFE/GTA) showed a liquid liquid (L-L) phase separation region, which is needed for a bicontinuous structure, prior to solid liquid (S-L) phase separation (polymer crystallization).
Both Rh and Gt were predominantly localized in the Ld phase, suggesting their low affinity to lipid rafts.
They display a locally anisotropic liquid phase referred to as "L phase" in a large temperature range between TNI and the low temperature SmQ or SmC∗A phase.
The morphologies of hollow fiber membranes were observed by scanning electron microscopy (SEM) and it was observed that a bicontinuous structure was formed through L-L phase separation.
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