The
emerging ferroelectric nematic (N
F
) liquid crystal is a novel 3D-ordered liquid exhibiting macroscopic
electric polarization. The combination of the ultrahigh dielectric
constant, strong nonlinear optical signal, and high sensitivity to
the electric field makes N
F
materials
promising for the development of advanced liquid crystal electroopic
devices. Previously, all studies focused on the rod-shaped small molecules
with limited length (l) range and dipole moment (μ)
values. Here, through the precision synthesis, we extend the aromatic
rod-shaped mesogen to oligomer/polymer (repeat unit up to 12 with
monodisperse molecular-weight dispersion) and increase the μ
value over 30 Debye (D). The N
F
phase has a widespread existence far beyond our expectation and
could be observed in all the oligomer/polymer length range. Notably,
the N
F
phase experiences a nontrivial
evolution pathway with the traditional apolar nematic phase completely
suppressed, i.e., the N
F
phase
nucleates directly from the isotropic liquid phase. The discovery
of thte ferroelectric packing of oligomer/polymer rods not only offers
the concept of extending the N
F
state to oligomers/polymers but also provides some previously overlooked
insights in oxybenzoate-based liquid crystal polymer materials.
The emerging ferroelectric nematic liquid crystals have been attracting broader interests in new liquid crystal physics and their unique material properties. One big challenge for the ferroelectric nematic researches is...
Second-order optical nonlinearity is the essential concept for realizing modern technologies of optical wavelength conversion. The emerging helical polarization fluid, dubbed helielectric nematic, now makes it possible to design and easily fabricate various polarization structures and control their optical responses. The matter family is demonstrated as an ideal liquid platform for nonlinear optical conversion and amplification with electric-reconfigurable tunability. We here develop a universal phase matching theory and reveal a nonclassic chirality-sensitive phase-matching condition in the polarization helices through both the numerical calculation and the experimental validations. The nonlinear optical amplification can be dramatically modulated with a contrast ratio of >100:1 by an in-plane electric field. Furthermore, we employ the director relaxation under electric fields coupled with nonlinear optical simulation to clarify the topology–light interactions.
The emerging matter category of liquid-matter ferroelectrics,
i.e.,
ferroelectric nematics, demonstrates an unprecedented combination
of fluidity and spontaneous polarization. However, unlike traditional
ferroelectrics, the field-switched polarization at zero-field cannot
be conserved, so the memory effect remains challenging. Here we report
another new type of ferroelectric liquid crystal state, dubbed the
ferroelectric smectic A phase, where the polarization is longitudinally
coupled to the smectic quasi-layer order. With higher packing density,
the phase exhibits higher values of refractive anisotropy and spontaneous
polarization compared to the ferroelectric nematics. A delicate balance
between the liquid crystal elasticity and flow viscosity enables both
the switching and memory of the polarization field, thus opening the
door toward realizing liquid-matter ferroelectric memory devices.
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