Abstract
Abstract We generalize the Rayleigh-Schrodinger perturbation formalism to the hamiltonians H = H 0 + λH 1 where the correction λH 1 is small and the unperturbed operator H 0 is represented by an infinite tridiagonal matrix. This enables us to construct the solutions E = E 0 + λE 1 + λ 2 E 2 +… and | ψ 〉 = | ψ 0 〉+ λ | ψ 1 〉+ λ 2 | ψ 2 〉+… in terms of the analytic continued fractions.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
