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PT-Symmetry in $2\times 2$ Matrix Polynomials Formed by Pauli Matrices

Mathematical Physics 2024-12-11 v2 math.MP

Abstract

2×22\times2 matrix polynomials of the form Pn(z)=Σj=0nσjzjP_{n}(z)= \Sigma^{n}_{j=0}\,\sigma_{j}\,z^{j}, for the cases n=1,2,3n=1,2,3 are constructed, and the nature of PT-symmetry is examined across different points z=(x,y)z=(x,y) in the complex plane. The PT-symmetric properties of Pn(z)P_{n}(z) can be characterized by two functions, denoted by s(x,y)s(x,y) and h(x,y)h(x,y). If the trace of the matrix polynomial is real, then the points at which it can exhibit PT-symmetry are defined by the family of curves s(x,y)=0s(x,y)=0. Additionally, at points where the function h(x,y)0h(x,y)\geq 0, the matrix polynomial exhibits unbroken PT-symmetry; otherwise, it exhibits broken PT-symmetry. The intersection points of the curves s(x,y)=0s(x,y)=0 and h(x,y)=kh(x,y)=k, for a given kRk\in \mathbb{R}, are shown to lie on an ellipse, hyperbola, two lines passing through the origin, or a straight line, depending on the nature of PT-symmetry of the matrix polynomial. The PT-symmetric behaviour of Pn(z)P_{n}(z) at the zeros of the matrix polynomial is also studied.

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Cite

@article{arxiv.2412.04022,
  title  = {PT-Symmetry in $2\times 2$ Matrix Polynomials Formed by Pauli Matrices},
  author = {Stalin Abraham and Ameeya A. Bhagwat},
  journal= {arXiv preprint arXiv:2412.04022},
  year   = {2024}
}

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