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Generating nonperturbative physics from perturbation theory
Phys. Rev. D 89, 041701(R) – Published 25 February, 2014
DOI: https://doi.org/10.1103/PhysRevD.89.041701
Abstract
In a large variety of quantum mechanical systems, we show that the full nonperturbative expression for energy eigenvalues, containing all orders of perturbative, nonperturbative, and quasi-zero-mode terms, may be generated directly from the perturbative expansion about the perturbative vacuum, combined with a single global boundary condition. This provides a dramatic realization of the principle of “resurgence,” that the fluctuations about different semiclassical saddle points are related to one another in a precise quantitative manner. The analysis of quantum mechanics also generalizes to certain calculable regimes of quantum field theory.
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References (26)
- C. M. Bender and T. T. Wu, Phys. Rev. 184, 1231 (1969); Phys. Rev. D 7, 1620 (1973).
- L. N. Lipatov, Zh. Eksp. Teor. Fiz. 72, 411 (1977) [Sov. Phys. JETP 45, 216 (1977)].
- J. Zinn-Justin, Quantum Field Theory and Critical Phenomena (Oxford University, New York, 2002).
- J. Zinn-Justin and U. D. Jentschura, Ann. Phys. (N.Y.) 313, 197 (2004); 313, 269 (2004); Phys. Lett. B 596, 138 (2004).
- P. C. Argyres and M. Ünsal, Phys. Rev. Lett. 109, 121601 (2012); J. High Energy Phys. 08 (2012) 063.
- G. V. Dunne and M. Ünsal, J. High Energy Phys. 11 (2012) 170; Phys. Rev. D 87, 025015 (2013).
- A. Cherman, D. Dorigoni, G. V. Dunne, and M. Unsal, Phys. Rev. Lett. 112, 021601 (2014).
- M. Ünsal and L. G. Yaffe, Phys. Rev. D 78, 065035 (2008).
- M. Mariño, R. Schiappa, and M. Weiss, Comm. Number Theor. Phys. 2, 349 (2008); M. Mariño, J. High Energy Phys. 12 (2008) 114; J. Phys. A 44, 463001 (2011).
- M. Mariño, arXiv:1206.6272.
- S. Pasquetti and R. Schiappa, Ann. Inst. Henri Poincaré 11, 351 (2010); I. Aniceto, R. Schiappa, and M. Vonk, Comm. Number Theor. Phys. 6, 339 (2012); I. Aniceto and R. Schiappa, arXiv:1308.1115; R. C. Santamara, J. D. Edelstein, R. Schiappa, and M. Vonk, arXiv:1308.1695.
- D. Krefl, arXiv:1311.0584.
- E. Brézin, G. Parisi, and J. Zinn-Justin, Phys. Rev. D 16, 408 (1977).
- M. Stone and J. Reeve, Phys. Rev. D 18, 4746 (1978).
- E. B. Bogomolny, Phys. Lett. 91B, 431 (1980).
- J. Zinn-Justin, Nucl. Phys. B192, 125 (1981); B218, 333 (1983); J. Math. Phys. (N.Y.) 25, 549 (1984).
- S. C. Miller and R. H. Good, Phys. Rev. 91, 174 (1953).
- NIST Digital Library of Mathematical Functions, http://dlmf.nist.gov/.
- G. V. Dunne and M. Ünsal, arXiv:1401.5202.
- G. Álvarez, J. Math. Phys. (N.Y.) 45, 3095 (2004).
- J. Zinn-Justin, J. Math. Phys. (N.Y.) 22, 511 (1981).
- C. F. Wöhler and E. V. Shuryak, Phys. Lett. B 333, 467 (1994).
- R. Dingle and H. Müller-Kirsten, J. Reine Angew. Math. 211, 11 (1962).
Note that the imaginary term is independent of the parity factor for the DW and of the Bloch angle for SG; this is crucial because these imaginary terms must cancel against terms coming from Borel summation of perturbation theory, and perturbation theory is independent of these parity and Bloch angle parameters.
- M. V. Berry and C. J. Howls, Proc. R. Soc. A 434, 657 (1991).
- G. Başar, G. V. Dunne, and M. Ünsal, J. High Energy Phys. 10 (2013) 041.