Euclidean Dynamical Triangulation revisited: is the phase transition really 1st order? (extended version)

TL;DR

This paper revisits the phase transition in 4D Euclidean Dynamical Triangulation, employing improved numerical methods to confirm its first-order nature and exploring modifications to potentially change its order.

Contribution

It introduces enhanced simulation techniques and a new theoretical framework to better understand the phase transition in EDT, challenging previous second-order assumptions.

Findings

Confirmed the phase transition is first order with improved methods

Developed a local criterion to distinguish triangulation states

Proposed modified measures to potentially alter the transition order

Abstract

The transition between the two phases of 4D Euclidean Dynamical Triangulation [1] was long believed to be of second order until in 1996 first order behavior was found for sufficiently large systems [5,9]. However, one may wonder if this finding was affected by the numerical methods used: to control volume fluctuations, in both studies [5,9] an artificial harmonic potential was added to the action; in [9] measurements were taken after a fixed number of accepted instead of attempted moves which introduces an additional error. Finally the simulations suffer from strong critical slowing down which may have been underestimated. In the present work, we address the above weaknesses: we allow the volume to fluctuate freely within a fixed interval; we take measurements after a fixed number of attempted moves; and we overcome critical slowing down by using an optimized parallel tempering algorithm [12]. With these improved methods, on systems of size up to 64k 4-simplices, we confirm that the phase transition is first order. In addition, we discuss a local criterion to decide whether parts of a triangulation are in the elongated or crumpled state and describe a new correspondence between EDT and the balls in boxes model. The latter gives rise to a modified partition function with an additional, third coupling. Finally, we propose and motivate a class of modified path-integral measures that might remove the metastability of the Markov chain and turn the phase transition into second order.