In this paper we analyze a recent application of perturbation theory by the moment method to a family of two-dimensional anharmonic oscillators. By means of straightforward unitary transformations we show that two of the models studied by the authors are separable. Other is unbounded from below and therefore cannot be successfully treated by perturbation theory unless a complex harmonic frequency is introduced in the renormalization process. We calculate the lowest resonance by means of complex-coordinate rotation and compare its real part with the eigenvalue estimated by the authors. A pair of the remaining oscillators are equivalent as they can be transformed into one another by unitary transformations.Fil: Fernández, Francisco Marcelo. C...
A recently-formulated residue-squaring method for perturbation problems is subjected to an exacting ...
This is the third article in a series of three papers on the resonance energy levels of anharmonic o...
A solution to the classical anharmonic-oscillator equation of motion x..=-x-λx2n-1 is obtained ...
We analyze earlier applications of perturbation theory by the moment method (also called inner produ...
Author Institution: Department of Chemistry, University of Calgary; Department of Chemistry, Univers...
To lowest order of perturbation theory we show that an equivalence can be established between a PT -...
We revisit the problem posed by an anharmonic oscillator with a potential given by a polynomial func...
This paper illustrates the application of group theory to a quantum-mechanical three-dimensional qua...
We use -after a shift transformation of the variable- the Burrows, Cohen and Feldmann approximation ...
We use -after a shift transformation of the variable- the Burrows, Cohen and Feldmann approximation ...
This paper illustrates the application of group theory to a quantum-mechanical three-dimensional qua...
The limits of current micro-scale technology is approaching rapidly. As the technology is going towa...
This paper illustrates the application of group theory to a quantum-mechanical three-dimensional qua...
We study the repulsive harmonic oscillator and an extension of this system, with an additional linea...
We use — after a shift transformation of the variable — the Burrows, Cohen and Feldmann approximati...
A recently-formulated residue-squaring method for perturbation problems is subjected to an exacting ...
This is the third article in a series of three papers on the resonance energy levels of anharmonic o...
A solution to the classical anharmonic-oscillator equation of motion x..=-x-λx2n-1 is obtained ...
We analyze earlier applications of perturbation theory by the moment method (also called inner produ...
Author Institution: Department of Chemistry, University of Calgary; Department of Chemistry, Univers...
To lowest order of perturbation theory we show that an equivalence can be established between a PT -...
We revisit the problem posed by an anharmonic oscillator with a potential given by a polynomial func...
This paper illustrates the application of group theory to a quantum-mechanical three-dimensional qua...
We use -after a shift transformation of the variable- the Burrows, Cohen and Feldmann approximation ...
We use -after a shift transformation of the variable- the Burrows, Cohen and Feldmann approximation ...
This paper illustrates the application of group theory to a quantum-mechanical three-dimensional qua...
The limits of current micro-scale technology is approaching rapidly. As the technology is going towa...
This paper illustrates the application of group theory to a quantum-mechanical three-dimensional qua...
We study the repulsive harmonic oscillator and an extension of this system, with an additional linea...
We use — after a shift transformation of the variable — the Burrows, Cohen and Feldmann approximati...
A recently-formulated residue-squaring method for perturbation problems is subjected to an exacting ...
This is the third article in a series of three papers on the resonance energy levels of anharmonic o...
A solution to the classical anharmonic-oscillator equation of motion x..=-x-λx2n-1 is obtained ...