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Nonlinear Bogolyubov-Valatin transformations: Two modes

机译:非线性Bogolyubov-Valatin转换:两种模式

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Extending our earlier study of nonlinear Bogolyubov-Valatin transformations (canonical transformations for fermions) for one fermionic mode, in the present paper, we perform a thorough study of general (nonlinear) canonical transformations for two fermionic modes. We find that the Bogolyubov-Valatin group for n=2 fermionic modes, which can be implemented by means of unitary SU(2n=4) transformations, is isomorphic to SO(6;R)R{double-struck}/Z{double-struck}_2. The investigation touches on a number of subjects. As a novelty from a mathematical point of view, we study the structure of nonlinear basis transformations in a Clifford algebra [specifically, in the Clifford algebra C(0,4)] entailing (supersymmetric) transformations among multivectors of different grades. A prominent algebraic role in this context is being played by biparavectors (linear combinations of products of Dirac matrices, quadriquaternions, sedenions) and spin bivectors (antisymmetric complex matrices). The studied biparavectors are equivalent to Eddington's E-numbers and can be understood in terms of the tensor product of two commuting copies of the division algebra of quaternions H{double-struck}. From a physical point of view, we present a method to diagonalize any arbitrary two-fermion Hamiltonians. Relying on Jordan-Wigner transformations for two-spin- 12 and single-spin- 32 systems, we also study nonlinear spin transformations and the related problem of diagonalizing arbitrary two-spin- 12 and single-spin- 32 Hamiltonians. Finally, from a calculational point of view, we pay due attention to explicit parametrizations of SU(4) and SO(6;R{double-struck}) matrices (of respective sizes 4×4 and 6×6) and their mutual relation.
机译:扩展了我们对一种费米子模态的非线性Bogolyubov-Valatin变换(费米子的规范变换)的早期研究,在本文中,我们对两种费米子模态的常规(非线性)规范变换进行了深入研究。我们发现,可以通过单一SU(2n = 4)转换实现的n = 2铁电离子模式的Bogolyubov-Valatin基团与SO(6; R)R {double-struck} / Z {double -struck} _2。该调查涉及多个主题。作为一种新颖的数学方法,我们研究了Clifford代数[特别是Clifford代数C(0,4)]中的非线性基础变换的结构,该变换要求在不同等级的多向量之间进行(超对称)变换。在这种情况下,双对向量(狄拉克矩阵,四元四元数,sedension的乘积的线性组合)和自旋双向量(反对称复矩阵)扮演着重要的代数角色。所研究的双对向量与爱丁顿的E数等效,并且可以根据四元数H {double-struck}的除法代数的两个换向副本的张量积来理解。从物理角度来看,我们提出了一种对角化任意二费米哈密顿量的方法。依靠两个自旋12和单自旋32系统的Jordan-Wigner变换,我们还研究了非线性自旋变换以及对角化任意两个自旋12和单自旋32哈密顿量的相关问题。最后,从计算角度出发,我们应适当注意SU(4)和SO(6; R {double-struck})矩阵(大小分别为4×4和6×6)的显式参数化及其相互关系。

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