2005
DOI: 10.1103/physreve.71.051701
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Telephone-cord instabilities in thin smectic capillaries

Abstract: Telephone-cord patterns have been recently observed in smectic liquid-crystal capillaries. We analyze the effects that may induce them. As long as the capillary keeps its linear shape, we show that a nonzero chiral cholesteric pitch favors the Sm-A*-Sm-C* transition. However, neither the cholesteric pitch nor the presence of an intrinsic bending stress is able to give rise to a curved capillary shape. The key ingredient for the telephone-cord instability is spontaneous polarization. The free-energy minimizer o… Show more

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Cited by 8 publications
(8 citation statements)
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References 24 publications
(28 reference statements)
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“…Magdeburg, Germany (Biscari and Calderer 2005;Bauman and Phillips 2009) and Kent, Ohio(Antal Jákli, Krüerke, and Nair 2003;T. Ostapenko et al 2014;Salili, Ostapenko, et al 2016) providing information on filament tensions and damping processes (Martin W. Schroder Gerhard Pelzl, and Wolfgang Weissflog 2004;Yao, Spiegelberg, and McKinley 2000;Stannarius, Nemeş, and Eremin 2005;Nemeş 2008;Nemeş et al 2006;Nemes, Eremin, and Stannarius 2006;Petzold et al 2009;Antal Jákli, Krüerke, and Nair 2003;Coleman et al 2003).…”
Section: Dynamical Properties Of Freely Suspended Liquid Crystal Filamentioning
confidence: 99%
“…Magdeburg, Germany (Biscari and Calderer 2005;Bauman and Phillips 2009) and Kent, Ohio(Antal Jákli, Krüerke, and Nair 2003;T. Ostapenko et al 2014;Salili, Ostapenko, et al 2016) providing information on filament tensions and damping processes (Martin W. Schroder Gerhard Pelzl, and Wolfgang Weissflog 2004;Yao, Spiegelberg, and McKinley 2000;Stannarius, Nemeş, and Eremin 2005;Nemeş 2008;Nemeş et al 2006;Nemes, Eremin, and Stannarius 2006;Petzold et al 2009;Antal Jákli, Krüerke, and Nair 2003;Coleman et al 2003).…”
Section: Dynamical Properties Of Freely Suspended Liquid Crystal Filamentioning
confidence: 99%
“…Suppose that K 2 , K 3 ≥ 8c 1 and 0 < |C ⊥ | 2Dq 2 ≤ 1. If (n, P, ω) is a minimizer of E, then the following estimates hold: ||(∇ω × n)|P| − P(|∇ω × n|)|| 2 2,Ω ≤ 2Ē 0 , (4.6)…”
Section: (43)mentioning
confidence: 98%
“…Modeling of static liquid crystal helical filaments can be found in [2,36]. Chevron structures with alternating domains of opposite polarization are also found in some materials [5].…”
mentioning
confidence: 98%
“…The energy of a smectic C liquid crystal may be written as the sum of a nematic energy term, which in the simplest approximation is the Frank energy (4), and a smectic term of the form (cf. [11], [15])…”
Section: Applications To Smectics Cmentioning
confidence: 99%