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Excess hyperpolarizabilities: the irreducible tensor approach

机译:过度极化率过高:张量方法不可约

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The irreducible spherical and Cartesian tensors built of the products of two interaction tensors: the second order tensor resulting from the product of two second order tensors ${{sf T}_{alpha,lambda},{sf T}_{lambda,beta}}$ contracted once with the index λ, third order tensor ${{sf T}_{alpha,beta,lambda} {sf T}_{lambda,gamma}}$ appearing as a product of the third order interaction tensor ${{sf T}_{alpha,beta,lambda}}$ and the second order one ${{sf T}_{lambda,gamma}}$ contracted once with the index λ and the fourth order product of two second order tensors ${{sf T}_{alpha,beta},{sf T}_{gammadelta}}$ , have been considered. This type of products is encountered, e.g., within the London’s dispersive energy formula, inside the second-order virial coefficients of many physical parameters such as the dielectric constant, the Kerr constant, the induced polarizability and hyperpolarizability of a pair of molecules and in other induced quantities. Our results are applied explicitly to the excess induced first and second pair hyperpolarizability.
机译:不可约的球形张量和笛卡尔张量由两个相互作用张量的乘积建立:由两个第二阶张量$ {{sf T} _ {alpha,lambda},{sf T} _ {lambda,beta }} $收缩一次,索引为λ,三阶张量$ {{sf T} _ {alpha,beta,lambda} {sf T} _ {lambda,gamma}} $作为三阶相互作用张量$的乘积出现{{sf T} _ {alpha,beta,lambda}} $和二阶一个$ {{sf T} _ {lambda,gamma}} $收缩一次,索引为λ,两个二阶张量的四阶乘积已考虑$ {{sf T} _ {alpha,beta},{sf T} _ {gammadelta}} $。例如,在伦敦的分散能公式中,许多物理参数(例如介电常数,克尔常数,一对分子的诱导极化率和超极化率)以及其他物理参数的二阶维里系数内都会遇到此类产品。诱导量。我们的结果明确地应用于过量诱导的第一对和第二对超极化率。

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