<p>In this paper we consider a two dimensional cholesteric liquid crystal with an applied external field, whose field configurations <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(u:\mathbb {R}^2\rightarrow S^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo stretchy="false">→</mo> <msup> <mi>S</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> are constant at infinity, and can be classified by their topological degree. We look for non trivial, topologically stable configurations (chiral skyrmions) by minimizing the Oseen-Frank energy functional over the functions <i>u</i> with <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\deg (u)=-1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>deg</mo> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. The energy functional depends on the splay (<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(K_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>K</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation>), twist (<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(K_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>K</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>) and bend (<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(K_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>K</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation>) elastic constants, and, assuming that <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(K_1=K_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>K</mi> <mn>1</mn> </msub> <mo>=</mo> <msub> <mi>K</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, we show the existence of skyrmions provided the cholesteric pitch <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(q_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>q</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> is small enough; moreover we study the compactness of such skyrmions as <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(q_0\rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>q</mi> <mn>0</mn> </msub> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and their limit. Our results generalize some previous results in the literature obtained under the assumption that <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(K_1=K_2=K_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>K</mi> <mn>1</mn> </msub> <mo>=</mo> <msub> <mi>K</mi> <mn>2</mn> </msub> <mo>=</mo> <msub> <mi>K</mi> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> (the well known “one-constant approximation” assumption). Moreover, in order to overcome the lack of compactness of the energy functional, we use (instead of the concentration-compactness principle) the fact that the field configurations with energy below a suitable threshold do not cover twice <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(S^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>S</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> minus a neighborhood of the North Pole, together with a truncation argument at infinity.</p>

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Skyrmions in two dimensional cholesteric liquid crystals

  • Carlo Greco

摘要

In this paper we consider a two dimensional cholesteric liquid crystal with an applied external field, whose field configurations \(u:\mathbb {R}^2\rightarrow S^2\) u : R 2 S 2 are constant at infinity, and can be classified by their topological degree. We look for non trivial, topologically stable configurations (chiral skyrmions) by minimizing the Oseen-Frank energy functional over the functions u with \(\deg (u)=-1\) deg ( u ) = - 1 . The energy functional depends on the splay ( \(K_1\) K 1 ), twist ( \(K_2\) K 2 ) and bend ( \(K_3\) K 3 ) elastic constants, and, assuming that \(K_1=K_2\) K 1 = K 2 , we show the existence of skyrmions provided the cholesteric pitch \(q_0\) q 0 is small enough; moreover we study the compactness of such skyrmions as \(q_0\rightarrow 0\) q 0 0 , and their limit. Our results generalize some previous results in the literature obtained under the assumption that \(K_1=K_2=K_3\) K 1 = K 2 = K 3 (the well known “one-constant approximation” assumption). Moreover, in order to overcome the lack of compactness of the energy functional, we use (instead of the concentration-compactness principle) the fact that the field configurations with energy below a suitable threshold do not cover twice \(S^2\) S 2 minus a neighborhood of the North Pole, together with a truncation argument at infinity.