Second-Order Perturbation in Adaptive Perturbation Method

Document Type : Regular article

Author

Asia Center for Theoretical Physics

Abstract

The perturbation method is an approximation scheme with a solvable leading order. The standard way is to choose a non-interacting sector for the leading order. The adaptive perturbation method improves the solvable part by using all diagonal elements for a Fock state. We consider the harmonic oscillator with the interacting term, λ1x4/6 + λ2x6/120, where λ1 and λ2 are coupling constants, and x  is the position operator. The spectrum shows a quantitative result from the second-order, less than 1 percent error, compared to a numerical solution when turning off the λ2. When we turn on the λ2, more deviation occurs, but the error is still less than 2 percent. We show a quantitative result beyond a weak-coupling region. Our study should provide interest in the holographic principle and strongly coupled boundary theory.

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[1] C. T. Ma, ”Parity Anomaly and Duality Web”, Fortsch. Phys. 66, 1800045 (2018).
[2] K. G. Wilson and M. E. Fisher, ”Critical exponents in 3.99 dimensions”, Phys. Rev. Lett. 28, 240-243 (1972).
[3] F. T. Hioe, D. Macmillen and E. W. Montroll, ”Quantum Theory of Anharmonic Oscillators: Energy Levels of a Single and a Pair of Coupled Oscillators with Quartic Coupling”, Phys. Rept. 43, 305-335 (1978).
[4] M. Weinstein, ”Adaptive perturbation theory. I. Quantum mechanics”, [arXiv:hep-th/0510159 [hep-th]].
[5] M. Weinstein, ”Adaptive perturbation theory: Quantum mechanics and field theory”, Nucl. Phys. B Proc. Suppl. 161, 238-247 (2006).
[6] F. Curcio, ”Metodi di approssimazione delle energie di sistemi unidimensionali conpotenziali polinomiali”, Tesi di Laurea Triennale (2017).
[7] C. T. Ma, ”Adaptive Perturbation Method in Quantum Mechanics”, IOP SciNotes 2, 035202 (2021).
Volume 2, Issue 4
November 2022
Pages 37-44
  • Receive Date: 12 August 2022
  • Revise Date: 26 September 2022
  • Accept Date: 28 September 2022