2021
DOI: 10.1016/j.molliq.2021.116816
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Influence of molecular weight on helical twisting power of oligomer chiral dopants

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Cited by 5 publications
(4 citation statements)
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“…The polymerization of mesogenic host (molecules 2 and 3 ) and the leaving of small molecular LC 6 result in a different LC host environment. The polymerization of chiral dopant 1 will decrease its HTP value, , while the leaving of nonpolymerizable chiral dopant 4 effectively increases the right-handed twisting effect. All these phenomena together determine the center wavelength the R-CPL reflection (Figure S4).…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The polymerization of mesogenic host (molecules 2 and 3 ) and the leaving of small molecular LC 6 result in a different LC host environment. The polymerization of chiral dopant 1 will decrease its HTP value, , while the leaving of nonpolymerizable chiral dopant 4 effectively increases the right-handed twisting effect. All these phenomena together determine the center wavelength the R-CPL reflection (Figure S4).…”
Section: Resultsmentioning
confidence: 99%
“…Inspired by the nature, scientists have been able to conceptualize versatile photonic architectures to provide appealing aesthetics and distinctive optical functions. , Tremendous efforts have been paid to engineer CLC materials or, more specifically, to control the helical organization of liquid crystal (LC) directors on the molecular scale. For instance, light-addressable or thermal-responsive chiral dopants allow tuning of the reflection wavelength. , Manipulation of the helical pitch direction or distribution provides an accessible route to realize beam steering, light diffraction, scattering, or broadband reflection. , Coupling helical structures of the opposite handedness can achieve hyper-reflectivity, defined as the ability to reflect both left- and right-handed circularly polarized light (L-CPL and R-CPL). In cross-linked CLC polymers, the distortion of helical structure generates polarization-dependent pseudo-Bragg reflectors and hyper-reflectivity. …”
Section: Introductionmentioning
confidence: 99%
“…When the pitch matches with the wavelength of light, a strong selective reflection occurs. According to the principle of the Bragg reflection, the central wavelength λ o and bandwidth Δ λ of the CLC reflection band can be represented as λ o = 〈 n 〉 p and Δ λ = Δ n · p , 29 where 〈 n 〉 and Δ n denote the average refractive index (〈 n 〉 = ( n e + n o )/2) and birefringence (Δ n = n e − n o ) of the CLC and p = 1/( βc ) is the helical pitch, 30 c is the concentration of the chiral dopant, and β is the helical twisting power.…”
Section: Methodsmentioning
confidence: 99%
“…When the pitch matches the wavelength of light, a strong selective reflection occurs. According to the principle of the Bragg reflection, the central wavelength λ o and bandwidth Δ λ of the CNLC reflection band can be represented as λ o = < n > p and Δ λ = Δ n ∙ p , 23 where < n > and Δ n denote the average refractive index (< n > = ( n e + n o )/2) and birefringence (Δ n = n e − n o ) of the CNLC, and p = 1/( βc ) is the helical pitch, 24 c is the concentration of the chiral dopant, and β is the helical twisting power.…”
Section: Methodsmentioning
confidence: 99%