1989
DOI: 10.1088/0305-4470/22/21/006
|View full text |Cite
|
Sign up to set email alerts
|

On tunnelling in the cubic potential

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
3
0

Year Published

1991
1991
2021
2021

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 9 publications
(5 citation statements)
references
References 5 publications
2
3
0
Order By: Relevance
“…For example, a potential in the form V = 1 2 mω 2 x 2 − 1 3 bx 3 can be used to model decay of metastable states [32], and it also describes the global flow [33]. Further, the tunnelling rate in real time in the semiclassical limit may be found for arbitrary energy levels, while it's ground state agrees well with the result found by the instanton method [34]. It is therefore worth continue the present study in view of such an additive form in the cubic potential.…”
Section: Power Law Potential F (φ) = φ Nsupporting
confidence: 70%
“…For example, a potential in the form V = 1 2 mω 2 x 2 − 1 3 bx 3 can be used to model decay of metastable states [32], and it also describes the global flow [33]. Further, the tunnelling rate in real time in the semiclassical limit may be found for arbitrary energy levels, while it's ground state agrees well with the result found by the instanton method [34]. It is therefore worth continue the present study in view of such an additive form in the cubic potential.…”
Section: Power Law Potential F (φ) = φ Nsupporting
confidence: 70%
“…For example, a potential in the form V = 1 2 mω 2 x 2 − 1 3 bx 3 can be used to model decay of metastable states [55], and it also describes the global flow [56]. Further, the tunnelling rate in real time in the semiclassical limit may be found for arbitrary energy levels, while its ground state agrees well with the result found by the instanton method [57]. It is therefore worth to continue the present study in view of such an additive form in the cubic potential.…”
Section: Case-2supporting
confidence: 69%
“…The first two terms in H m are the potential energy and the kinetic energy of the simple harmonic oscillator, respectively, the third term involving q 3 is the potential energy produced by the cubic mechanical nonlinearity, the parameter α is the strength of the mechanical nonlinearity. It is noted that many aspects of a cubic nonlinear oscillator have been studied, such as the behavior of the resonances [37], the quantum mechanical tunnelling [38], the Bender-Wu branch points [39], the real spectrum [40], the Stark effect [41], the periodic motion [42], and the homoclinic bifurcation [43]. Moreover, in the adiabatic limit of ω m πc/L (c is the speed of light in vacuum, L is the length of the cavity), the oscillation of the movable mirror is very slow, thus the scattering of the photons to the other cavity modes can be neglected, so there is only one cavity mode in the cavity [44].…”
Section: Modelmentioning
confidence: 99%