In physics, Landau–de Gennes theory describes the NI transition, i.e., phase transition between nematic liquid crystals and isotropic liquids, which is based on the classical Landau's theory and was developed by Pierre-Gilles de Gennes in 1969. The phenomenological theory uses the Q {\displaystyle \mathbf {Q} } tensor as an order parameter in expanding the free energy density.
Mathematical description The NI transition is a first-order phase transition, albeit it is very weak. The order parameter is the Q {\displaystyle \mathbf {Q} } tensor, which is symmetric, traceless, second-order tensor and vanishes in the isotropic liquid phase. We shall consider a uniaxial Q {\displaystyle \mathbf {Q} } tensor, which is defined by
Q = S ( n ⊗ n − 1 3 I ) {\displaystyle \mathbf {Q} =S(\mathbf {n} \otimes \mathbf {n} -{\tfrac {1}{3}}\mathbf {I} )}
where S = S ( T ) {\displaystyle S=S(T)} is the scalar order parameter and n {\displaystyle \mathbf {n} } is the director. The Q {\displaystyle \mathbf {Q} } tensor is zero in the isotropic liquid phase since the scalar order parameter S {\displaystyle S} is zero, but becomes non-zero in the nematic phase. Near the NI transition, the (Helmholtz or Gibbs) free energy density F {\displaystyle {\mathcal {F}}} is expanded about as
F = F 0 + A 2 Q i j Q j i − B 3 Q i j Q j k Q k i + C 4 ( Q i j Q i j ) 2 {\displaystyle {\mathcal {F}}={\mathcal {F}}_{0}+{\frac {A}{2}}Q_{ij}Q_{ji}-{\frac {B}{3}}Q_{ij}Q_{jk}Q_{ki}+{\frac {C}{4}}(Q_{ij}Q_{ij})^{2}}
or more compactly
F = F 0 + A 2 t r Q 2 − B 3 t r Q 3 + C 4 ( t r Q 2 ) 2 {\displaystyle {\mathcal {F}}={\mathcal {F}}_{0}+{\frac {A}{2}}\mathrm {tr} \,\mathbf {Q} ^{2}-{\frac {B}{3}}\mathrm {tr} \,\mathbf {Q} ^{3}+{\frac {C}{4}}(\mathrm {tr} \,\mathbf {Q} ^{2})^{2}}
where ( A , B , C ) {\displaystyle (A,B,C)} are functions of temperature. Near the phase transition, we can expand A ( T ) = a ( T − T ∗ ) + ⋯ {\displaystyle A(T)=a(T-T_{*})+\cdots } , B ( T ) = b + ⋯ {\displaystyle B(T)=b+\cdots } and C ( T ) = c + ⋯ {\displaystyle C(T)=c+\cdots } with ( a , b , c ) {\displaystyle (a,b,c)} being three positive constants. Now substituting the Q {\displaystyle \mathbf {Q} } tensor results in
F − F 0 = a 3 ( T − T ∗ ) S 2 − 2 b 27 S 3 + c 9 S 4 . {\displaystyle {\mathcal {F}}-{\mathcal {F}}_{0}={\frac {a}{3}}(T-T_{*})S^{2}-{\frac {2b}{27}}S^{3}+{\frac {c}{9}}S^{4}.}
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