Complementarity vs coordinate transformations: Mapping between pseudo-Hermiticity and weak pseudo-Hermiticity

نویسندگان

چکیده

\noindent We study the concept of complementarity, introduced by Bagchi and Quesne in [Phys. Lett. A {\bf 301}, 173 (2002)], between pseudo-Hermiticity weak a rigorous mathematical viewpoint coordinate transformations when system has position-dependent mass. first determine, under modified-momentum, generating functions identifying complexified potentials $V_\pm(x)$ both concepts $\widetilde\eta_+$ (resp. $\widetilde\eta_-$). show that complementarity can be understood interpreted as transformation through their respective functions. As consequence, similarity which implements is obtained. set up fundamental relationship connecting $\widetilde\eta_-$. special factorization $\eta_+=\eta_-^\dagger \eta_-$ discussed case constant mass some B\"acklund are derived.

برای دانلود رایگان متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Pseudo-Hermiticity, weak pseudo-Hermiticity and η-orthogonality condition

We discuss certain features of pseudo-Hermiticity and weak pseudo-Hermiticity conditions and point out that, contrary to a recent claim, there is no inconsistency if the correct orthogonality condition is used for the class of pseudo-Hermitian, PTsymmetric Hamiltonians of the type Hβ = [p + iβν(x)] 2/2m + V (x). PACS: 03.65.Ca

متن کامل

Is Weak Pseudo-Hermiticity Weaker than Pseudo-Hermiticity?

For a weakly pseudo-Hermitian linear operator, we give a spectral condition that ensures its pseudo-Hermiticity. This condition is always satisfied whenever the operator acts in a finite-dimensional Hilbert space. Hence weak pseudo-Hermiticity and pseudo-Hermiticity are equivalent in finite-dimensions. This equivalence extends to a much larger class of operators. Quantum systems whose Hamiltoni...

متن کامل

QT -Symmetry and Weak Pseudo-Hermiticity

For an invertible (bounded) linear operator Q acting in a Hilbert space H, we consider the consequences of the QT -symmetry of a non-Hermitian Hamiltonian H : H → H where T is the time-reversal operator. If H is symmetric in the sense that THT = H, then QT symmetry is equivalent toQ-weak-pseudo-Hermiticity. But in general this equivalence does not hold. We show this using some specific examples...

متن کامل

η-weak-pseudo-Hermiticity generators and radially symmetric Hamiltonians

A class η-weak-pseudo-Hermiticity generators for spherically symmetric non-Hermitian Hamiltonians are presented. An operators-based procedure is introduced so that the results for the 1D Schrödinger Hamiltonian may very well be reproduced. A generalization beyond the nodeless states is proposed. Our illustrative examples include η-weak-pseudo-Hermiticity generators for the non-Hermitian weakly ...

متن کامل

η-weak-pseudo-Hermiticity generators per exact solvability

Exact solvability of some non-Hermitian η-weak-pseudo-Hermitian Hamiltonians is explored as a byproduct of η-weak-pseudo-Hermiticity generators. A class of Veff (x) = V (x) + iW (x) potentials is considered, where the imaginary part W (x) is used as an η-weak-pseudo-Hermiticity generator to obtain exactly solvable η-weak-pseudo-Hermitian Hamiltonian models. PACS numbers: 03.65.Ge, 03.65.Fd,03.6...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

ژورنال

عنوان ژورنال: Journal of Mathematical Physics

سال: 2021

ISSN: ['0022-2488', '1527-2427', '1089-7658']

DOI: https://doi.org/10.1063/5.0036401