Timeline of computational physics The following timeline starts with the invention of the modern computer in the late interwar period .1930s John Vincent Atanasoff and Clifford Berry create the first electronic non-programmable, digital computing device, the Atanasoff–Berry Computer , that lasted from 1937 to 1942.1940s Nuclear bomb and ballistics simulations at Los Alamos and BRL, respectively. Monte Carlo simulation is invented at Los Alamos by von Neumann , Ulam and Metropolis. First hydrodynamic simulations performed at Los Alamos. Ulam and von Neumann introduce the notion of cellular automata .1950s Equations of State Calculations by Fast Computing Machines introduces the Metropolis–Hastings algorithm . Also, important earlier independent work by Alder and S. Frankel. Fermi, Ulam and Pasta with help from Mary Tsingou , discover the Fermi–Pasta–Ulam problem . Research initiated into percolation theory . Molecular dynamics is formulated by Alder and Wainwright.1960s Using computational investigations of the 3-body problem , Minovitch formulates the gravity assist method. Glauber dynamics is invented for the Ising model . Edward Lorenz discovers the butterfly effect on a computer, attracting interest in chaos theory . Molecular dynamics is independently invented by Aneesur Rahman . W Kohn instigates the development of density functional theory , for which he shared the Nobel Chemistry Prize . Kruskal and Zabusky follow up the Fermi–Pasta–Ulam problem with further numerical experiments, and coin the term "soliton". Kawasaki dynamics is invented for the Ising model. Frenchman Verlet discovers a numerical integration algorithm , for dynamics, and the Verlet list .1970s Computer algebra replicates the work of Delaunay in Lunar theory . Veltman's calculations at CERN lead him and t'Hooft to valuable insights into Renormalizability of Electroweak theory . The computation has been cited as a key reason for the award of the Nobel prize that has been given to both. Hardy, Pomeau and de Pazzis introduce the first lattice gas model , abbreviated as the HPP model after its authors. These later evolved into lattice Boltzmann models. Wilson shows that continuum QCD is recovered for an infinitely large lattice with its sites infinitesimally close to one another, thereby beginning lattice QCD .1980s Italian physicists Car and Parrinello invent the Car–Parrinello method . Swendsen–Wang algorithm is invented in the field of Monte Carlo simulations . Fast multipole method is invented by Rokhlin and Greengard. U. Wolff invents the Wolff algorithm for statistical physics and Monte Carlo simulation.
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