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Mathematical rules of reasonable expectation
Proposition A: The Condensed Matter group Christmas dinner is on Tuesday evening. Proposition B: Turnout at this week's Theory Club is low. If A implies B, Aristotle would tell us that the only logical deduction we can make is that a high attendance
01 | Medical Informatics | Usher Connects | Usher Institute
First floor | Winter Garden 1
Monto Carlo simulation and extended sampling
No details are available for this event.
RACE.ED Archival Research Fellowships | IASH
The Centre for Research Collections (CRC) is the main space for anyone using the University of Edinburgh’s cultural and heritage collections.
Philip Golding | Fundraise Your Way | Giving
A colleague's devastating diagnosis inspired Philip to run 1,000 km in 2022.
Mechanics and geometry of growing tissues
The mechanical properties of biological tissues are generally studied either at a macroscopic level by considering the tissue as a liquid (with a non-conserved number of cells) or at a microscopic cellular level by a vertex model that considers
Complex-tensor theory of simple smectics
The same properties that make smectic phases so interesting concomitantly contrive to make them challenging to model. They're interesting becacuse they are excellent systems for exploring self-assembly and topology since they accommodate both
The Lieb-Yngvason theory of thermodynamics
The structure of thermodynamics follows from the existence of an extensive, additive, and concave entropy function. Yet despite the centrality of entropy in the theory, it is often introduced in a roundabout way via heat engines, or by invoking
Dynamical fluctuation theory in a nutshell
A dynamical fluctuation is an atypical value of a time-integrated observable such as entropy production, particle current, or number of state transitions in a stochastic system. A comprehensive theory exists for how to characterize the likelihood of
Dynamic condensates in aggregation processes
The Takayasu aggregation model is a model of aggregation with mass injection, known to exhibit a power law distribution of mass $\sim \frac{1}{m^\tau}$ with $\tau = \frac{4}{3}$ in 1D, over a mass range which grows in time. It is a paradigmatic
