Carl M. Bender
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View article: Complex phases in quantum mechanics
Complex phases in quantum mechanics Open
Schrödinger's equation is a local differential equation and boundary conditions are required to determine the solution uniquely. Depending on the choice of boundary conditions, a given Hamiltonian may describe several different physically …
View article: Complex phases in quantum mechanics
Complex phases in quantum mechanics Open
Hamilton's equations of motion are local differential equations and boundary conditions are required to determine the solution uniquely. Depending on the choice of boundary conditions, a Hamiltonian may thereby describe several different p…
View article: New Classes of Solutions for Euclidean Scalar Field Theories
New Classes of Solutions for Euclidean Scalar Field Theories Open
This paper presents new classes of exact radial solutions to the nonlinear ordinary differential equation that arises as a saddle-point condition for a Euclidean scalar field theory in D-dimensional spacetime. These solutions are found by …
View article: PT-symmetric quantum mechanics
PT-symmetric quantum mechanics Open
It is generally assumed that a Hamiltonian for a physically acceptable quantum system (one that has a positive-definite spectrum and obeys the requirement of unitarity) must be Hermitian. However, a PT-symmetric Hamiltonian can also define…
View article: Dyson-Schwinger equations in zero dimensions and polynomial approximations
Dyson-Schwinger equations in zero dimensions and polynomial approximations Open
The Dyson-Schwinger (DS) equations for a quantum field theory in $D$-dimensional space-time are an infinite sequence of coupled integro-differential equations that are satisfied exactly by the Green's functions of the field theory. This se…
View article: New classes of solutions for Euclidean scalar field theories
New classes of solutions for Euclidean scalar field theories Open
This paper presents new classes of exact radial solutions to the nonlinear ordinary differential equation that arises as a saddle-point condition for a Euclidean scalar field theory in $D$-dimensional spacetime. These solutions are found b…
View article: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi mathvariant="script">P</mml:mi><mml:mi mathvariant="script">T</mml:mi></mml:mrow></mml:math>-symmetric<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mo>−</mml:mo><mml:mi>g</mml:mi><mml:msup><mml:mrow><mml:mi>φ</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>theory
-symmetrictheory Open
The scalar field theory with potential $V(\varphi)=\textstyle{\frac{1}{2}} m^2\varphi^2-\textstyle{\frac{1}{4}} g\varphi^4$ ($g>0$) is ill defined as a Hermitian theory but in a non-Hermitian $\mathcal{P}\mathcal{T}$-symmetric framework it…
View article: Underdetermined Dyson-Schwinger equations
Underdetermined Dyson-Schwinger equations Open
This paper examines the effectiveness of the Dyson-Schwinger (DS) equations as a calculational tool in quantum field theory. The DS equations are an infinite sequence of coupled equations that are satisfied exactly by the connected Green's…
View article: $\mathcal{P}\mathcal{T}$-symmetric $-gφ^4$ theory
$\mathcal{P}\mathcal{T}$-symmetric $-gφ^4$ theory Open
The scalar field theory with potential $V(φ)=\textstyle{\frac{1}{2}} m^2φ^2-\textstyle{\frac{1}{4}} gφ^4$ ($g>0$) is ill defined as a Hermitian theory but in a non-Hermitian $\mathcal{P}\mathcal{T}$-symmetric framework it is well defined, …
View article: Experimentally-realizable $\mathcal{PT}$ phase transitions in reflectionless quantum scattering
Experimentally-realizable $\mathcal{PT}$ phase transitions in reflectionless quantum scattering Open
A class of above-barrier quantum-scattering problems is shown to provide an experimentally-accessible platform for studying $\mathcal{PT}$-symmetric Schrödinger equations that exhibit spontaneous $\mathcal{PT}$ symmetry breaking despite ha…
View article: Towards perturbative renormalization of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi>ϕ</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo stretchy="false">(</mml:mo><mml:mi>i</mml:mi><mml:mi>ϕ</mml:mi><mml:msup><mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mi>ϵ</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:math>quantum field theory
Towards perturbative renormalization ofquantum field theory Open
In a previous paper it was shown how to calculate the ground-state energy density $E$ and the $p$-point Green's functions $G_p(x_1,x_2,...,x_p)$ for the $PT$-symmetric quantum field theory defined by the Hamiltonian density $H=\frac{1}{2}(…
View article: PT symmetry and renormalisation in quantum field theory
PT symmetry and renormalisation in quantum field theory Open
Quantum systems governed by non-Hermitian Hamiltonians with symmetry are special in having real energy eigenvalues bounded below and unitary time evolution. We argue that symmetry may also be important and present at the level of Her…
View article: PT -symmetric classical mechanics
PT -symmetric classical mechanics Open
This paper reports the results of an ongoing in-depth analysis of the classical trajectories of the class of non-Hermitian -symmetric Hamiltonians H = p 2 + x 2 ( ix ) ε ( ε ⩾ 0). A variety of phenomena, heret…
View article: Fourth Painlevé Equation and $PT$-Symmetric Hamiltonians
Fourth Painlevé Equation and $PT$-Symmetric Hamiltonians Open
This paper is an addendum to earlier papers \cite{R1,R2} in which it was shown that the unstable separatrix solutions for Painlevé I and II are determined by $PT$-symmetric Hamiltonians. In this paper unstable separatrix solutions of the f…
View article: $PT$-symmetric classical mechanics
$PT$-symmetric classical mechanics Open
This paper reports the results of an ongoing in-depth analysis of the classical trajectories of the class of non-Hermitian $PT$-symmetric Hamiltonians $H=p^2+ x^2(ix)^\varepsilon$ ($\varepsilon\geq0$). A variety of phenomena, heretofore ov…
View article: PT -symmetric quantum field theory
PT -symmetric quantum field theory Open
-symmetric quantum theory began with an analysis of the strange-looking non-Hermitian Hamiltonian H = p 2 + x ( ix ) ε . This Hamiltonian is symmetric and the eigenvalues Hamiltonian are discrete, real, and positive when ε ≥ 0. In this …
View article: PT-symmetric potentials having continuous spectra
PT-symmetric potentials having continuous spectra Open
One-dimensional PT-symmetric quantum-mechanical Hamiltonians having continuous spectra are studied. The Hamiltonians considered have the form $H=p^2+V(x)$, where $V(x)$ is odd in $x$, pure imaginary, and vanishes as $|x|\to\infty$. Five PT…
View article: Relativistic <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi mathvariant="script">PT</mml:mi></mml:math>-symmetric fermionic theories in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mn>3</mml:mn><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:math> dimensions
Relativistic -symmetric fermionic theories in and dimensions Open
Relativistic PT-symmetric fermionic interacting systems are studied in 1+1\nand 3+1 dimensions. The objective is to include non-Hermitian PT-symmetric\ninteraction terms that give {\\it real} spectra. Such interacting systems could\ndescri…
View article: Nonlinear eigenvalue problems for generalized Painlevé equations
Nonlinear eigenvalue problems for generalized Painlevé equations Open
Eigenvalue problems for linear differential equations, such as\ntime-independent Schr\\"odinger equations, can be generalized to eigenvalue\nproblems for nonlinear differential equations. In the nonlinear context a\nseparatrix plays the ro…
View article: Operator-valued zeta functions and Fourier analysis
Operator-valued zeta functions and Fourier analysis Open
The Riemann zeta function Ϛ(s) is defined as the infinite sum
\n∑∞n=1n-s, which
\nconverges when Re s ˃ 1. The Riemann hypothesis asserts that the nontrivial zeros
\nof Ϛ(s)…
View article: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi mathvariant="script">P</mml:mi><mml:mi mathvariant="script">T</mml:mi></mml:mrow></mml:math>-symmetric quantum field theory in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>D</mml:mi></mml:math> dimensions
-symmetric quantum field theory in dimensions Open
PT-symmetric quantum mechanics began with a study of the Hamiltonian H=p2+x2(ix)μ. A surprising feature of this non-Hermitian Hamiltonian is that its eigenvalues are discrete, real, and positive when μ≥0. This paper examines the correspond…
View article: Scattering off <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi mathvariant="script">P</mml:mi><mml:mi mathvariant="script">T</mml:mi></mml:mrow></mml:math>-symmetric upside-down potentials
Scattering off -symmetric upside-down potentials Open
The upside-down $-x^4$, $-x^6$, and $-x^8$ potentials with appropriate\nPT-symmetric boundary conditions have real, positive, and discrete\nquantum-mechanical spectra. This paper proposes a straightforward macroscopic\nquantum-mechanical s…
View article: PT Symmetry
PT Symmetry Open
The ideas of PT symmetry were originally introduced in the context of quantum mechanics, but in recent years they have led to rapid developments in the apparently unconnected field of classical optics ...
View article: Asymptotic analysis of the local potential approximation to the Wetterich equation
Asymptotic analysis of the local potential approximation to the Wetterich equation Open
This paper reports a study of the nonlinear partial differential equation\nthat arises in the local potential approximation to the Wetterich formulation\nof the functional renormalization group equation. A cut-off-dependent shift of\nthe p…
View article: Two- and four-dimensional representations of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi mathvariant="script">PT</mml:mi></mml:math>- and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi mathvariant="script">CPT</mml:mi></mml:math>-symmetric fermionic algebras
Two- and four-dimensional representations of the - and -symmetric fermionic algebras Open
Fermionic systems differ from their bosonic counterparts, the main difference with regard to symmetry considerations being that $T^2=-1$ for fermionic systems. In PT-symmetric quantum mechanics an operator has both PT and CPT adjoints. Fer…
View article: Asymptotic analysis on a pseudo-Hermitian Riemann-zeta Hamiltonian
Asymptotic analysis on a pseudo-Hermitian Riemann-zeta Hamiltonian Open
The differential-equation eigenvalue problem associated with a recently-introduced Hamiltonian, whose eigenvalues correspond to the zeros of the Riemann zeta function, is analyzed using Fourier and WKB analysis. The Fourier analysis leads …
View article: Physics in the Complex Domain
Physics in the Complex Domain Open
first_page settings Order Article Reprints Font Type: Arial Georgia Verdana Font Size: Aa Aa Aa Line Spacing: Column Width: Background: Open AccessAbstract Physics in the Complex Domain † by Carl M. Bender Physics Department, W…
View article: Winding in non-Hermitian systems
Winding in non-Hermitian systems Open
This paper extends the property of interlacing of the zeros of eigenfunctions\nin Hermitian systems to the topological property of winding number in\nnon-Hermitian systems. Just as the number of nodes of each eigenfunction in a\nself-adjoi…
View article: Two-Dimensional Pulse Propagation without Anomalous Dispersion
Two-Dimensional Pulse Propagation without Anomalous Dispersion Open
Anomalous dispersion is a surprising phenomenon associated with wave propagation in an even number of space dimensions. In particular, wave pulses propagating in two-dimensional space change shape and develop a tail even in the absence of …
View article: Nonlinear eigenvalue problems and<i>PT</i>-symmetric quantum mechanics
Nonlinear eigenvalue problems and<i>PT</i>-symmetric quantum mechanics Open
Semiclassical (WKB) techniques are commonly used to find the large-energy behavior of the eigenvalues of linear time-independent Schrödinger equations. In this talk we generalize the concept of an eigenvalue problem to nonlinear differenti…