In mathematics and physics, a non-perturbative function or process is one that cannot be described by perturbation theory. An example is the function

The function e−1/x2. The MacLaurin series is identically zero, but the function is not.

which does not equal its own Taylor series in any neighborhood around x = 0. Every coefficient of the Taylor expansion around x = 0 is exactly zero, but the function is non-zero if x ≠ 0.

In physics, such functions arise for phenomena which are impossible to understand by perturbation theory, at any finite order. In quantum field theory, 't Hooft–Polyakov monopoles, ___domain walls, flux tubes, and instantons are examples.[1] A concrete, physical example is given by the Schwinger effect,[2] whereby a strong electric field may spontaneously decay into electron-positron pairs. For not too strong fields, the rate per unit volume of this process is given by,

which cannot be expanded in a Taylor series in the electric charge , or the electric field strength . Here is the mass of an electron and we have used units where .

In theoretical physics, a non-perturbative solution is one that cannot be described in terms of perturbations about some simple background, such as empty space. For this reason, non-perturbative solutions and theories yield insights into areas and subjects that perturbative methods cannot reveal.

See also

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References

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  1. ^ Shifman, M. (2012). Advanced Topics in Quantum Field Theory. Cambridge University Press. ISBN 978-0-521-19084-8.
  2. ^ Schwinger, Julian (1951-06-01). "On Gauge Invariance and Vacuum Polarization". Physical Review. 82 (5). American Physical Society (APS): 664–679. doi:10.1103/physrev.82.664. ISSN 0031-899X.