scholarly journals RAPID TUNNELING AND PERCOLATION IN THE LANDSCAPE

2009 ◽  
Vol 24 (04) ◽  
pp. 741-788 ◽  
Author(s):  
SASWAT SARANGI ◽  
GARY SHIU ◽  
BENJAMIN SHLAER

Motivated by the possibility of a string landscape, we re-examine tunneling of a scalar field across single/multiple barriers. Recent investigations have suggested modifications to the usual picture of false vacuum decay that leads to efficient and rapid tunneling in the landscape when certain conditions are met. This can be due to stringy effects (e.g. tunneling via the DBI action), or effects arising from the presence of multiple vacua (e.g. resonance tunneling). In this paper we discuss both DBI tunneling and resonance tunneling. We provide a QFT treatment of resonance tunneling using the Schrödinger functional approach. We also show how DBI tunneling for supercritical barriers can naturally lead to conditions suitable for resonance tunneling. We argue, using basic ideas from percolation theory, that tunneling can be rapid in a landscape where a typical vacuum has multiple decay channels, and discuss various cosmological implications. This rapidity vacuum decay can happen even if there are no resonance/DBI tunneling enhancements, solely due to the presence of a large number of decay channels. Finally, we consider various ways of circumventing a recent no-go theorem for resonance tunneling in quantum field theory.

2018 ◽  
Vol 177 ◽  
pp. 09001 ◽  
Author(s):  
Maxim Bezuglov

When the Higgs boson was discovered in 2012 it was realized that electroweak vacuum may suffer a possible metastability on the Planck scale and can eventually decay. To understand this problem it is important to have reliable predictions for the vacuum decay rate within the framework of quantum field theory. For now, it can only be done at one loop level, which is apparently is not enough. The aim of this work is to develop a technique for the calculation of two and higher order radiative corrections to the false vacuum decay rate in the framework of four dimensional scalar quantum field theory and then apply it to the case of the Standard Model. To achieve this goal, we first start from the case of d=1 dimensional QFT i.e. quantum mechanics. We show that for some potentials two and three loop corrections can be very important and must be taken into account. Next, we use quantum mechanical example as a template for the general d=4 dimensional theory. In it we are concentrating on the calculations of bounce solution and corresponding Green function in so called thin wall approximation. The obtained Green function is then used as a main ingredient for the calculation of two loop radiative corrections to the false vacuum decay rate.


2001 ◽  
Vol 64 (10) ◽  
Author(s):  
Esteban Calzetta ◽  
Albert Roura ◽  
Enric Verdaguer

2016 ◽  
Vol 25 (07) ◽  
pp. 1642008 ◽  
Author(s):  
Wolfgang Bietenholz

We sketch the basic ideas of the lattice regularization in Quantum Field Theory, the corresponding Monte Carlo simulations, and applications to Quantum Chromodynamics (QCD). This approach enables the numerical measurement of observables at the non-perturbative level. We comment on selected results, with a focus on hadron masses and the link to Chiral Perturbation Theory. At last, we address two outstanding issues: topological freezing and the sign problem.


2001 ◽  
Vol 88 (1) ◽  
Author(s):  
Esteban Calzetta ◽  
Albert Roura ◽  
Enric Verdaguer

Author(s):  
Paul Teller

Quantum field theory extends the basic ideas of quantum mechanics for a fixed, finite number of particles to systems comprising fields and an unlimited, indefinite number of particles, providing a coherent blend of field-like and particle-like concepts. One can start from either field- or particle-like concepts, apply the methods of quantum mechanics, and arrive at the same theory. The result inherits all the puzzles of conventional quantum mechanics, such as measurement, superposition and quantum correlations; and it adds a new roster of conceptual difficulties. To mention three: the vacuum seems not really to be empty; the particle concept clashes with classical intuitions; and a method called ‘renormalization’ gets the best predictions in physics, apparently by dropping infinite terms.


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