Discrete-coordinate crypto-Hermitian quantum system controlled by
time-dependent Robin boundary conditions
- URL: http://arxiv.org/abs/2401.10682v2
- Date: Wed, 31 Jan 2024 06:57:20 GMT
- Title: Discrete-coordinate crypto-Hermitian quantum system controlled by
time-dependent Robin boundary conditions
- Authors: Miloslav Znojil
- Abstract summary: unitary quantum mechanics formulated in non-Hermitian (or, more precisely, in hiddenly Hermitian) interaction-picture representation is illustrated via an elementary $N$ by $N$ matrix Hamiltonian $H(t)$ mimicking a 1D-box system with physics controlled by time-dependent boundary conditions.
Our key message is that contrary to the conventional beliefs and in spite of the unitarity of the evolution of the system, neither its "Heisenbergian Hamiltonian" $Sigma(t)$ nor its "Schr"odingerian Hamiltonian" $G(
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: Non-stationary version of unitary quantum mechanics formulated in
non-Hermitian (or, more precisely, in hiddenly Hermitian) interaction-picture
representation is illustrated via an elementary $N$ by $N$ matrix Hamiltonian
$H(t)$ mimicking a 1D-box system with physics controlled by time-dependent
boundary conditions. The model is presented as analytically solvable at $N=2$.
Expressis verbis, this means that for both of the underlying Heisenbergian and
Schr\"{o}dingerian evolution equations the generators (i.e., in our notation,
the respective operators $\Sigma(t)$ and $G(t)$) become available in closed
form. Our key message is that contrary to the conventional beliefs and in spite
of the unitarity of the evolution of the system, neither its "Heisenbergian
Hamiltonian" $\Sigma(t)$ nor its "Schr\"{o}dingerian Hamiltonian" $G(t)$
possesses a real spectrum or the conjugate pairs of complex eigenvalues. This
means that neither one of these "Hamiltonians" can be pseudo-Hermitian alias
PT-symmetric.
Related papers
- Slow Mixing of Quantum Gibbs Samplers [47.373245682678515]
We present a quantum generalization of these tools through a generic bottleneck lemma.
This lemma focuses on quantum measures of distance, analogous to the classical Hamming distance but rooted in uniquely quantum principles.
Even with sublinear barriers, we use Feynman-Kac techniques to lift classical to quantum ones establishing tight lower bound $T_mathrmmix = 2Omega(nalpha)$.
arXiv Detail & Related papers (2024-11-06T22:51:27Z) - Zig-zag-matrix algebras and solvable quasi-Hermitian quantum models [0.0]
We conjecture that the role of the diagonalized-matrix solution of the quantum bound-state problem could be transferred to a maximally sparse zig-zag-matrix'' representation of the Hamiltonians.
arXiv Detail & Related papers (2023-07-07T07:51:47Z) - Non-stationary non-Hermitian "wrong-sign'' quantum oscillators and their
meaningful physical interpretation [0.0]
Quantum mechanics of closed, unitary quantum systems can be formulated in non-Hermitian interaction picture.
Only the sum $H(t)=G(t)+Sigma(t)$ retains the standard physical meaning of instantaneous energy.
arXiv Detail & Related papers (2023-04-14T12:52:15Z) - Composite quantum Coriolis forces [0.0]
Coriolis force finds its quantum analogue in the difference $Sigma(t)=H(t)-G(t)$ where the true'', observable Hamiltonian $H(t)$ represents the instantaneous energy.
The other, false'' Hamiltonian $G(t)$ generates the time-evolution of wave functions.
arXiv Detail & Related papers (2023-03-07T22:18:20Z) - Systematics of quasi-Hermitian representations of non-Hermitian quantum
models [0.0]
This paper introduces and describes a set of constructive returns of the description to one of the correct and eligible physical Hilbert spaces $cal R_N(0)$.
In the extreme of the theory the construction is currently well known and involves solely the inner product metric $Theta=Theta(H)$.
At $j=N$ the inner-product metric remains trivial and only the Hamiltonian must be Hermitized, $H to mathfrakh = Omega,H,Omega-1=mathfrak
arXiv Detail & Related papers (2022-12-07T20:10:58Z) - Hybrid form of quantum theory with non-Hermitian Hamiltonians [0.0]
Freeman Dyson discovered that the practical solution of Schr"odinger equation may be facilitated when one replaces the standard self-adjoint Hamiltonian $mathfrakh=mathfrakhdagger$.
In our present letter we describe an alternative Hermitization of a hybrid form'' which simply combines the OT model-building strategy with the MA model-building strategy.
arXiv Detail & Related papers (2022-11-19T09:51:29Z) - Geometric relative entropies and barycentric Rényi divergences [16.385815610837167]
monotone quantum relative entropies define monotone R'enyi quantities whenever $P$ is a probability measure.
We show that monotone quantum relative entropies define monotone R'enyi quantities whenever $P$ is a probability measure.
arXiv Detail & Related papers (2022-07-28T17:58:59Z) - The Franke-Gorini-Kossakowski-Lindblad-Sudarshan (FGKLS) Equation for
Two-Dimensional Systems [62.997667081978825]
Open quantum systems can obey the Franke-Gorini-Kossakowski-Lindblad-Sudarshan (FGKLS) equation.
We exhaustively study the case of a Hilbert space dimension of $2$.
arXiv Detail & Related papers (2022-04-16T07:03:54Z) - On quantum algorithms for the Schr\"odinger equation in the
semi-classical regime [27.175719898694073]
We consider Schr"odinger's equation in the semi-classical regime.
Such a Schr"odinger equation finds many applications, including in Born-Oppenheimer molecular dynamics and Ehrenfest dynamics.
arXiv Detail & Related papers (2021-12-25T20:01:54Z) - Boundary time crystals in collective $d$-level systems [64.76138964691705]
Boundary time crystals are non-equilibrium phases of matter occurring in quantum systems in contact to an environment.
We study BTC's in collective $d$-level systems, focusing in the cases with $d=2$, $3$ and $4$.
arXiv Detail & Related papers (2021-02-05T19:00:45Z) - A map between time-dependent and time-independent quantum many-body
Hamiltonians [23.87373187143897]
Given a time-independent Hamiltonian $widetilde H$, one can construct a time-dependent Hamiltonian $H_t$ by means of the gauge transformation $H_t=U_t widetilde H, Udagger_t-i, U_t, partial_t U_tdagger$.
Here $U_t$ is the unitary transformation that relates the solutions of the corresponding Schrodinger equations.
arXiv Detail & Related papers (2020-09-29T08:54:21Z)
This list is automatically generated from the titles and abstracts of the papers in this site.
This site does not guarantee the quality of this site (including all information) and is not responsible for any consequences.