Abstract

The Airy distribution (AD) describes the probability distribution of the area under a Brownian excursion. The AD is prominent in several areas of physics, mathematics and computer science. Here we use a dilute colloidal system to directly measure, for the first time, the AD in experiment. We also show how two different techniques of theory of large deviations - the Donsker-Varadhan formalism and the optimal fluctuation method - manifest themselves in the AD. We advance the theory of the AD by calculating, at large and small areas, the position distribution of a Brownian excursion conditioned on a given area, and measure its mean in the experiment. For large areas, we uncover two singularities in the large deviation function, which can be interpreted as dynamical phase transitions of third order. For small areas the position distribution coincides with the Ferrari-Spohn distribution, and we identify the reason for this coincidence.

Highlights

  • Brownian motion came to prominence in physics and other sciences with the theoretical works of Einstein [1], von Smoluchowski [2], and Langevin [3] and the experimental work of Perrin [4]

  • We show how two different techniques of theory of large deviations, the Donsker-Varadhan formalism and the optimal fluctuation method, manifest themselves in the Airy distribution (AD)

  • We advance the theory of the AD by calculating, at large and small areas, the position distribution of a Brownian excursion conditioned on a given area and measure its mean in the experiment

Read more

Summary

This distribution exhibits the scaling behavior

The full position distribution of excursions, conditioned on a given area, requires a considerably larger number of trajectories. For the small-area simulations, in the window A = 0.3 ± 0.0075, we used 1885 trajectories These were extracted from a total of 2 × 106 unconditioned Brownian excursions. We verified the simulation method by measuring the area distribution of the excursions and comparing the results with the theoretical predictions (2) and (3).

The effective Schrödinger equation for the Brownian excursion reads
The SCGF is given by
The path integral that corresponds to the FS model is
The distribution of X is given by
Dimensional analysis yields the scaling form
Calculating the action from

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.