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Micellar solution between two cross polarizers with a stainless steel planar lab spatula dipping into the liquid. Prior to introducing the stainless steel spatula, the fluid is dark since light cannot pass through as in an isotropic fluid. However, as the spatula is introduced into the liquid, the fluid flows, as a result of the applied shear, and birefringence is clearly observed.

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Birefringence pattern of a colloid suspension of the filamentous virus fd seen by polarization microscopy showing a cholesteric phase

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L2_L"2 phase transition in the C21 fatty acid monolayer at T=2.2 °C and lateral pressure of 5.3 mN/m. The L2 is the phase before the transition, and after the front of change passes, we observe the L''2. Image width ~850 μm.

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Localized oscillations (interference rings blinking) in the crystalline phases of C21 fatty acid monolayer at temperatures close to 2 °C. Image widh ~850 μm.

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Pattern of growth of a condensed phase from a liquid expanded phase in the ethyl stearate monolayer, at 32 C. The transition from tip-splitting to side branching is clearly observed.

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Shear induced structures (SIS) in worm-like micellar solutions during a thixotropic loop at high shear rates (original speed of the film was reduced at half). Bright stripes formed by bundles of strong interacting worm-like micelles are observed by light scattering in a sheared fluid placed in the gap of a transparent Couette cell.

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Dismantling of shear induced structures (SIS) in worm-like micellar solutions during a thixotropic loop (down-shear curve). Bright stripes formed by bundles of strong interacting worm-like micelles are observed by light scattering in a sheared fluid placed in the gap of a transparent Couette cell.

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Formation of shear induced structures (SIS) in worm-like micellar solutions during a thixotropic loop (up-shear curve). Bright stripes formed by bundles of strong interacting worm-like micelles are observed by light scattering in a sheared fluid placed in the gap of a transparent Couette cell.

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