Critical Points at Infinity, Non-Gaussian Saddles, and Bions
Mar 30, 2018
30 pages
Published in:
- JHEP 06 (2018) 068
- Published: Jun 13, 2018
e-Print:
- 1803.11533 [hep-th]
Report number:
- NSF-ITP-18-007
View in:
Citations per year
Abstract: (Springer)
It has been argued that many non-perturbative phenomena in quantum mechanics (QM) and quantum field theory (QFT) are determined by complex field configurations, and that these contributions should be understood in terms of Picard-Lefschetz theory. In this work we compute the contribution from non-BPS multi-instanton configurations, such as instanton-anti-instanton pairs, and argue that these contributions should be interpreted as exact critical points at infinity. The Lefschetz thimbles associated with such critical points have a specific structure arising from the presence of non-Gaussian, quasi-zero mode (QZM), directions. When fermion degrees of freedom are present, as in supersymmetric theories, the effective bosonic potential can be written as the sum of a classical and a quantum potential. We show that in this case the semi-classical contribution of the critical point at infinity vanishes, but there is a non-trivial contribution that arises from its associated non-Gaussian QZM-thimble. This approach resolves several puzzles in the literature concerning the semi-classical contribution of correlated pairs. It has the surprising consequence that the configurations dominating the expansion of observables, and the critical points defining the Lefschetz thimble decomposition need not be the same, a feature not present in the traditional Picard-Lefschetz approach.Note:
- 31 pages, v2: fixed hyperlinks to references, minor edits
- Nonperturbative Effects
- Differential and Algebraic Geometry
- Resummation
- potential: quantum
- boson: potential
- critical phenomena
- field theory
- non-Gaussianity
- quantum mechanics
- nonperturbative
References(60)
Figures(6)
- [1]
- [2]
- [3]
- [4]
- [5]
- [6]
- [7]
- [8]
- [9]
- [10]
- [11]
- [12]
- [13]
- [14]
- [15]
- [16]
- [17]
- [18]
- [19]
- [20]
- [21]
- [22]
- [23]
- [24]
- [25]