Duda Jarek Posted September 3, 2020 Share Posted September 3, 2020 (edited) To choose random walk on a graph, it seems natural to to assume that the walker jumps using each possible edge with the same probability (1/degree) - such GRW (generic random walk) maximizes entropy locally (for each step). Discretizing continuous space and taking infinitesimal limit we get various used diffusion models. However, looking at mean entropy production: averaged over stationary probability distribution of nodes, its maximization leads to usually a bit different MERW: https://en.wikipedia.org/wiki/Maximal_entropy_random_walk It brings a crucial question which philosophy should we choose for various applications - I would like to discuss. GRW - uses approximation of (Jaynes) https://en.wikipedia.org/wiki/Principle_of_maximum_entropy - has no localization property (nearly uniform stationary probability distribution), - has characteristic length of one step - this way e.g. depends on chosen discretization of a continuous system. MERW - is the one maximizing mean entropy, "most random among random walks", - has strong localization property - stationary probability distribution exactly as quantum ground state, - is limit of characteristic step to infinity - is discretization independent. Simulator of both for electron conductance: https://demonstrations.wolfram.com/ElectronConductanceModelsUsingMaximalEntropyRandomWalks/ Diagram with example of evolution and stationary denstity, also some formulas (MERW uses dominant eigenvalue): Edited September 3, 2020 by Duda Jarek 1 Link to comment Share on other sites More sharing options...
studiot Posted September 3, 2020 Share Posted September 3, 2020 4 hours ago, Duda Jarek said: I would like to discuss. Nice topic +1 But. Beware of confusing random progression through a mathematical graph with a spatial random walk for say a gaseous molecule. Link to comment Share on other sites More sharing options...
Duda Jarek Posted September 3, 2020 Author Share Posted September 3, 2020 (edited) Thanks, my general thoughts is that: GRW should be used when the walker directly uses the assumed random walk, like "drunken sailor" throwing a dice in each node, or just human making looking random local decisions which link to click at for https://en.wikipedia.org/wiki/PageRank - it is for walkers performing nearly random decisions accordingly to local situation, having characteristic length like one web link. MERW stochastic propagator is nonlocal - depends on the entire space (in eigenequation of adjacency matrix) - it shouldn't be seen as directly used by the walker. Instead, this is thermodynamical picture - the safest (entropy maximizing) assumption we can make for limited knowledge situations like some complex hidden dynamics e.g. in electron conductance. Edited September 3, 2020 by Duda Jarek Link to comment Share on other sites More sharing options...
studiot Posted September 3, 2020 Share Posted September 3, 2020 Hidden beneath all those big words and phrases is the fact that the random walks described are more like drunk wandering the grid pattern of streets at night. He takes a 'random' decision at each intersection but is constrained as to the four directions he can take. Furthermore it does not matter how much time he takes deciding or walking. This is a single discrete random variable. A gaseous particle, on the other hand does not take decisions. Its random walk come from being buffetted by other particles in a random fashion. This random fashion occurs at random instants, imparting random momenta in random directions. All of these three variables are fully continuous independent random variables. 1 Link to comment Share on other sites More sharing options...
Duda Jarek Posted September 3, 2020 Author Share Posted September 3, 2020 Exactly, GRW is perfect e.g. for human wandering through the web, indeed performing local randomly looking decisions. MERW for electrons - having extremely complex EM&wave-based dynamics, expressing our limited knowledge through its entropy maximization, with Anderson-like localization property e.g. preventing semiconductor from being a conductor, like in below electron densities from STM (scanning tunneling microscope) from http://www.phy.bme.hu/~zarand/LokalizacioWeb/Yazdani.pdf The big question is what to choose between, like for this molecular dynamics? Practical difference is that only MERW has QM-like localization property - do we observe this kind of effects for molecules? Like entropic boundary avoidance, e.g. for [0,1] range GRW/diffusion/chaos would predict nearly uniform rho=1 stationary distribution, while QM/MERW predicts rho~sin^2 distribution avoiding boundaries - do we observe it for molecules? Link to comment Share on other sites More sharing options...
dimreepr Posted September 3, 2020 Share Posted September 3, 2020 40 minutes ago, Duda Jarek said: GRW is perfect e.g. for human wandering through the web, indeed performing local randomly looking decisions. I think the point is, GRW is a random choice in a bounded enviroment; which becomes more bounded (and less random) with each subsequent decision. Link to comment Share on other sites More sharing options...
Duda Jarek Posted September 3, 2020 Author Share Posted September 3, 2020 It is also crucial that it is local random choice: based on possible single steps, having characteristic length like use of single step. MERW can be seen as scale-free limit of GRW_k: using uniform (/Boltzmann) distribution of length k paths from given position: GRW = GRW_1 MERW = lim_{k->infty} GRW_k Link to comment Share on other sites More sharing options...
Recommended Posts
Create an account or sign in to comment
You need to be a member in order to leave a comment
Create an account
Sign up for a new account in our community. It's easy!
Register a new accountSign in
Already have an account? Sign in here.
Sign In Now